Method of, and apparatus for, transmitting energy

ABSTRACT

Invention for transmitting energy in an effective manner for applications comprising cold nuclear fusion, radiosurgery, radiotherapy, non-invasive ophthalmic surgery, imaging, power transmission, communications, energy storage, momentum-based power generation, and data storage and retrieval comprising:
         Step 1) providing apparatus for producing a beam of electromagnetically neutralized energy comprising electromagnetic wave-particle behaving entities comprising waves which destructively interfere to an extent, and associated electromagnetic fields which cancel to a respective extent; and,   Step 2) coherent transmission of the beam of electromagnetically neutralized energy by coherent transmission apparatus to a target. Wherein, adverse electromagnetic interaction of the coherently transmitted beam of electromagnetically neutralized energy with electrically charged particles in the coherent transmission apparatus is eliminated to an extent, thus eliminating an extent of the overall adverse electromagnetic effect of transmitting energy. Hence, energy is transmitted in an effective manner to the target to accomplish the objective of the present invention.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. (1) shows a plan side view of a generalized drawing of a preferredembodiment of the present invention which is applied for transmittingenergy in an effective manner in which a beam of electromagneticallyneutralized wave-particle behaving entities is applied.

FIG. (2) shows a plan side view of a somewhat more specific preferredembodiment of the present invention that is applied for transmittingenergy in an effective manner which is different by applying a beam oftotally electromagnetically neutralized wave-particle behaving entities.

FIG. (3) shows the construction of one version of a beam ofelectromagnetically neutralized wave-particle behaving entitiescomprising a beam of totally electromagnetically neutralizedwave-particle behaving entities.

FIG. (4) shows a pulsed beam of totally electromagnetically neutralizedwave-particle behaving entities which is another version of a beam oftotally electromagnetically neutralized wave-particle behaving entities.

FIG. (5) shows a digitally pulse modulated beam of totallyelectromagnetically neutralized wave-particle behaving entities thatencodes data which is another version of a beam of totallyelectromagnetically neutralized wave-particle behaving entities.

FIG. (6) shows a plan side view of another somewhat more specificpreferred embodiment of the present invention that is applied fortransmitting energy in an effective manner which is different byapplying a beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities.

FIG. (7) shows a beam of partly electromagnetically neutralized andpartly electromagnetically functional wave-particle behaving entitieswhich is another version of a beam of electromagnetically neutralizedwave-particle behaving entities.

FIG. (8) shows a pulsed beam of partly electromagnetically neutralizedand partly electromagnetically functional wave-particle behavingentities which is another version of a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities.

FIG. (9) shows a digitally pulse modulated beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities which is another version of abeam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities.

FIG. (10) shows a plan side view of a somewhat generalized preferredembodiment which is applied for the transmission and subsequentutilization of momentum in an effective manner.

FIG. (11) shows a plan side view of another somewhat generalizedpreferred embodiment that is applied for the transmission and subsequentutilization of energy in an effective manner which is different byapplying a beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities in aparticular manner.

FIG. (12) shows a plan side view of another somewhat generalizedpreferred embodiment that is applied for the transmission and subsequentutilization of energy in an effective manner which is different byapplying a beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entitiescomprising polarized beam portions/components in a particular manner.

FIG. (13) shows a plan side view of another somewhat generalizedpreferred embodiment that is applied for the transmission and subsequentutilization of energy in an effective manner which is different byapplying a beam of electromagnetically neutralized wave-particlebehaving entities in a particular manner.

FIG. (14) shows a plan side view of another somewhat generalizedpreferred embodiment that is applied for the transmission and subsequentutilization of energy in an effective manner which is different byapplying a beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities inanother particular manner.

FIG. (15) shows a plan side view of another somewhat generalizedpreferred embodiment that is applied for the transmission and subsequentutilization of energy in an effective manner which is different byapplying a beam of electromagnetically neutralized wave-particlebehaving entities in yet another particular manner.

FIG. (16) shows a plan side view of another somewhat generalizedpreferred embodiment that is applied for the transmission and subsequentutilization of energy in an effective manner which is different byapplying a beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities in stillyet another particular manner.

FIG. (17) shows a plan side view of a somewhat generalized conditionalpreferred embodiment that is applied for the transmission and subsequentutilization of energy in an effective manner which is different byapplying certain steps dependent upon which apparatus, including whichtype of beam of electromagnetically neutralized wave-particle behavingentities, is applied.

FIG. (18) shows a plan side view of another somewhat generalizedpreferred embodiment that is applied for the transmission and subsequentutilization of energy in an effective manner which is different byapplying a beam of electromagnetically neutralized wave-particlebehaving entities and a target comprising utilizing apparatus locatedposteriorly.

FIG. (19) shows a plan side view of another somewhat generalizedpreferred embodiment that is applied for the transmission and subsequentutilization of energy in an effective manner which is different byapplying a beam of electromagnetically neutralized wave-particlebehaving entities and a target comprising utilizing apparatus located atsome anterior or lateral location in the target.

FIG. (20) shows a plan side view of another somewhat generalizedpreferred embodiment which is applied for the transmission andsubsequent utilization of energy in an effective manner which isdifferent by applying a beam of electromagnetically neutralizedwave-particle behaving entities and combining steps applied in otherpreferred embodiments.

FIG. (21) shows a plan side view of another somewhat generalizedpreferred embodiment that is applied for the transmission and subsequentutilization of energy in an effective manner which is different byapplying a beam of electromagnetically neutralized wave-particlebehaving entities that comprises electromagnetically neutralizedwave-particle behaving entities which individually and collectivelycomprise potential energy so to effectively produce incoherentlyscattering apparatus at a focus in a target.

FIG. (22) shows a plan side view of another somewhat generalizedpreferred embodiment that is applied for the transmission and subsequentutilization of energy in an effective manner which is different byapplying another beam as an incoherently scattering apparatus.

FIG. (23) is another preferred embodiment which is applied for thetransmission of energy in an effective manner which is different byapplying a filtering apparatus.

FIG. (24) shows a plan side view of a generalized preferred embodimentof the present invention which is surrounded by shielding apparatus.

FIG. (25) shows two embodiments of the present invention which togetherrepresent the significance of adjusting the particle flux density of abeam of totally electromagnetically neutralized wave-particle behavingentities.

FIG. (26) shows two embodiments of the present invention which togetherrepresent the significance of adjusting the particle flux density of abeam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities.

FIG. (27) shows two embodiments of the present invention which togetherrepresent one aspect of the significance of adjusting the time-averageelectric flux density of the present invention.

FIG. (28) shows two embodiments of the present invention which togetherrepresent another aspect of the significance of adjusting thetime-average electric flux density of the present invention.

FIG. (29) shows two embodiments of the present invention which togetherrepresent the significance of adjusting the position of the focal pointof the present invention.

FIG. (30) shows a plan side view of a generalized preferred embodimentof the present invention which is applied for efficient cold nuclearfusion.

FIG. (31) shows a plan side view of a generalized preferred embodimentof the present invention for performing radiological treatment (e.g.,radiosurgery or radiotherapy) in an effective manner.

FIG. (32) shows a plan side view of a somewhat more specific preferredembodiment which is applied for performing radiological treatment in aneffective manner by applying a focused beam of electromagneticallyneutralized wave-particle behaving entities in a hard treatment site.

FIG. (33) shows a plan side view of another somewhat more specificpreferred embodiment which is applied for performing radiologicaltreatment in an effective manner by applying a focused beam ofelectromagnetically neutralized wave-particle behaving entities in asoft treatment site (e.g., a soft organic tumor) which is locatedposterior to hard media (comprising hard potential-energy-typeincoherently scattering media comprising electrically charged particles)which may or may not be part of the treatment site, while, necessarily,the treatment site comprises the soft treatment site located posteriorto (beyond) the hard media.

FIG. (34) shows the radiological arrangement of a somewhat more specificpreferred embodiment which is applied for performing radiologicaltreatment in an effective manner by applying a focused beam ofelectromagnetically neutralized wave-particle behaving entities in ahard treatment site (e.g., a calcified tumor) which is surrounded bysoft healthy brain tissue located in the brain of a surgically preparedpatient.

FIG. (34A) is an enlarged view of a section within the treatment site inthe preferred embodiment for performing radiological treatment shown inFIG. (34) which shows the focused beam of electromagneticallyneutralized wave-particle behaving entities in soft healthy brain tissueand projecting into in the hard treatment site, and shows the incoherentbeam of electromagnetically functional wave-particle behaving entitiesproduced in the hard treatment site.

FIG. (35) shows the radiological arrangement of another somewhat morespecific preferred embodiment which is applied for performingradiological treatment in an effective manner by performing radiologicaltreatment of a soft treatment site (e.g., a soft organic tumor) which islocated posterior to hard media (comprising hard potential-energy-typeincoherently scattering media comprising electrically charged particles)which may or may not be part of the treatment site; while, necessarily,the treatment site comprises the soft treatment site located posteriorto (beyond) the hard media in the brain of a surgically preparedpatient.

FIG. (35A) is an enlarged view of a section within the treatment site inthe preferred embodiment for performing radiation treatment shown inFIG. (35) which shows the focused beam of electromagneticallyneutralized wave-particle behaving entities in soft healthy brain tissueand projecting into in the hard treatment media, and shows theincoherent beam of electromagnetically functional wave-particle behavingentities produced in the posteriorly located soft treatment site.

FIG. (36) shows a plan side view of another somewhat more specificpreferred embodiment which is applied for performing radiologicaltreatment in an effective manner by applying a focused beam ofelectromagnetically neutralized wave-particle behaving entities in abone.

FIG. (37) shows a plan side view of another somewhat more specificpreferred embodiment which is applied for performing radiologicaltreatment in an effective manner by applying a focused beam ofelectromagnetically neutralized wave-particle behaving entities in abone comprising hard potential-energy-type incoherently scattering mediacomprising electrically charged particles which may or may not be partof the treatment site, while, necessarily, the treatment site is a softtreatment site comprised in the bone marrow located posterior to(beyond) the given bone.

FIG. (38) shows a plan side view of another somewhat more specificpreferred embodiment for performing radiation treatment in an effectivemanner which is different by applying a beam of electromagneticallyneutralized wave-particle behaving entities which is broad and a hardtreatment site which is large.

FIG. (39) shows a plan side view of another somewhat specific preferredembodiment that is applied for performing radiotherapy in an effectivemanner which is different by applying a beam of electromagneticallyneutralized wave-particle behaving entities which is broad and atreatment site which comprises a plurality of small hard treatmentsites.

FIG. (40) shows the radiological arrangement of another somewhat morespecific preferred embodiment that is applied for performingradiological treatment in an effective manner which is different byapplying a focused beam of electromagnetically neutralized wave-particlebehaving electrons of sufficiently high energy (i.e., non-refractingelectrons), which individually and collectively comprise potentialenergy in order to effectively produce incoherently scattering apparatus(comprising potential-energy-type incoherently scattering apparatus) ina soft treatment site (e.g., an organic tumor) in the brain of asurgically prepared patient.

FIG. (41A) is an enlarged view of a section within the treatment site ofthe preferred embodiment for radiation treatment shown in FIG. (41)which shows the focused beam of electromagnetically neutralizedelectrons in the soft healthy brain tissue and in the soft treatmentsite, and shows the incoherent beam of electromagnetically functionalwave-particle behaving entities produced in the soft treatment site.

FIG. (42) shows a plan side view of a somewhat narrowly scoped andgeneralized preferred embodiment of the present invention which isapplied for performing non-invasive ophthalmic surgery in an effectivemanner.

FIG. (43) shows the surgical arrangement of the present invention fornon-invasive ophthalmic surgery of a patient by an ophthalmic surgeon.

FIG. (44) shows a plan side view of a generalized preferred embodimentof the present invention which is applied for performing atransmissive-type of imaging in an effective manner.

FIG. (45) shows a plan side view of another generalized preferredembodiment of the present invention which is applied for performing abackscattering-type of imaging in an effective manner.

FIG. (46) includes a longitudinally sectioned view of the tubing of aside view of a somewhat generalized preferred embodiment of the presentinvention which is applied for efficiently transmitting power.

FIG. (47) includes a longitudinally sectioned view of the tubing of aside view of another preferred embodiment of the present invention thatis applied for efficiently transmitting power which is different byapplying tubing as a splitter.

FIG. (48) includes a longitudinally sectioned view of the tubing of aside view of another preferred embodiment of the present invention thatis applied for efficiently transmitting power which is different byapplying tubing as a coupler.

FIG. (49) includes a longitudinally sectioned view of the tubing of aside view of another preferred embodiment of the present invention thatis applied for efficiently transmitting power which is different byapplying tubing as a splitter and a coupler.

FIG. (50) shows a plan side view of a somewhat generalized preferredembodiment of the present invention that is applied for efficientwireline-type communications which applies tubing for signaltransmission.

FIG. (51) shows a plan side view of a somewhat generalized preferredembodiment of the present invention that is applied for efficientwireless-type communications which applies air for signal transmission.

FIG. (52) shows a plan side view of a somewhat more specific preferredembodiment of the present invention that is applied for efficientwireless-type communications which is different by applying a beamcomprising combined polarized beam portions.

FIG. (53) shows a plan side view of another somewhat more specificpreferred embodiment of the present invention that is applied forefficient wireline-type communications which is different by applyingwave division multiplexing and demultiplexing.

FIG. (53A) shows somewhat yet more specific preferred embodiment appliedfor efficient wireline-type communications which is different byapplying prisms for wave division multiplexing and demultiplexing.

FIG. (53B) shows yet another somewhat more specific preferred embodimentof the present invention applied for efficient wireless-typecommunications which is different by applying diffraction gratings forwave division multiplexing and demultiplexing.

FIG. (54) shows yet another somewhat more specific preferred embodimentof the present invention which is applied for efficient wireless-typecommunications which is different by applying air for coherenttransmission media instead of tubing.

FIG. (55) shows another preferred embodiment of the present inventionapplied for efficient wireless-type communications which is different byapplying a beam comprising combined polarized beam portions and wavedivision multiplexing and demultiplexing.

FIG. (56) shows a preferred embodiment of the present invention which isapplied for efficient energy storage and subsequent utilization.

FIG. (56A) shows a perspective view of the basic shape of the energystorage container which is applied in the preferred embodiment of thepresent invention shown in FIG. (56).

FIG. (57) shows a plan top view of a preferred embodiment of the presentinvention which is applied for efficient momentum-based voltagegeneration.

FIG. (58) shows another preferred embodiment of the present inventionthat is applied for efficient momentum-based voltage generation which isdifferent by applying additional apparatus, comprising additionalMichelson interferometric apparatus, additional beams of totallyelectromagnetically neutralized electromagnetic field quanta, andadditional pressure transducers, for producing additional momentum-basedvoltage generation.

FIG. (59) shows a preferred embodiment of the present invention that isapplied for efficient power generation which applies a load to amomentum-based voltage generator in order to produce momentum-basedpower generation.

FIG. (60) shows a preferred embodiment of the present invention which isapplied for efficient data storage and retrieval.

FIG. (61) is a sectional view of another preferred embodiment of thepresent invention applied for data storage and retrieval in an efficientmanner which is different by applying additional apparatus, comprisingadditional Michelson interferometric apparatus, additional beams oftotally electromagnetically neutralized electromagnetic field quanta,and additional pressure transducers, in order to comprise a higher datastorage and retrieval capacity.

FIG. (61A) exclusively shows one Michelson interferometric apparatus andrespective beams of electromagnetic field quanta in the formation of abeam of totally electromagnetically neutralized electromagnetic fieldquanta in more detailed in an enlarged view of a section of thepreferred embodiment for data storage and retrieval shown in FIG. (61).

FIG. (62) shows another preferred embodiment of the present inventionapplied for data storage and retrieval in an efficient manner which isdifferent by applying a frequency division type of multiplexed beams oftotally electromagnetically neutralized electromagnetic field quanta anda plurality of transducers for respective demultiplexing.

DESCRIPTION

The present invention is described for transmitting energy in somegeneralized preferred embodiments including descriptions of some ways anembodiment of the present invention can be adjusted to accomplish arespective objective. Also, more specifically, the present invention isdescribed in preferred embodiments for transmitting energy inapplications comprising cold nuclear fusion, radiosurgery, radiotherapy,non-invasive ophthalmic surgery, imaging, power transmission,communications, energy storage, momentum-based power generation, anddata storage and retrieval. (Note, refer to the notes at the end of thisdetailed description for clarification of the terms applied herein.)

FIG. (1) shows a plan side view of a generalized drawing of a preferredembodiment of the present invention which is applied for transmittingenergy (per se) in an effective manner. The preferred embodiment in FIG.(1) is applied as follows:

Step 1) apparatus (2), comprising apparatus which produces a coherentbeam of electromagnetic wave-particle behaving entities andinterferometric apparatus (e.g., the Michelson interferometric apparatusas respectively applied in the preferred embodiments in FIGS. (56),(58), (62-62C) and (63), produces a beam of electromagneticallyneutralized wave-particle behaving entities (4) (which is continuous orpulsed, collimated or focused, and linearly, circularly, elliptically,or unpolarized). The beam of electromagnetically neutralizedwave-particle behaving entities (4) comprises, as examples, a beam ofelectromagnetically neutralized wave-particle behaving electromagneticfield quanta or a beam of electromagnetically neutralized wave-particlebehaving electrically charged particles comprising the same electriccharge, i.e., beam of electromagnetically neutralized propagatingprotons or electrons).

More specifically, the beam of electromagnetically neutralizedwave-particle behaving entities (4) comprises electromagneticwave-particle behaving entities which each comprise an oscillatorytime-varying electromagnetic field with an associated wave, totalenergy, and momentum. (Note, electromagnetic wave-particle behavingentities refers to the group of wave-particle behaving entities whichparticipate in electromagnetic interaction.)

The given beam of electromagnetically neutralized wave-particle behavingentities (4) comprises coherent waves superimposed out of phase to anextent so to produce destructive interference to an extent, such thatthe respective oscillatory time-varying electromagnetic fields in beam(4) cancel to a respective extent. Wherein, the electromagneticwave-particle behaving entities in the beam of electromagneticallyneutralized wave-particle behaving entities (4) are electromagneticallyneutralized in direct proportion to the time-average electric fluxdensity which is eliminated from the beam of electromagneticallyneutralized wave-particle behaving entities (4) (Note, a beam ofelectromagnetically neutralized wave-particle behaving entities cancomprise a beam of totally electromagnetically neutralized wave-particlebehaving entities produced by total destructive interference of wavesand total cancellation of associated time-varying electric and magneticfields, respectively, or a beam of electromagnetically neutralizedwave-particle behaving entities can comprise a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities produced by partialdestructive interference of waves and partial cancellation of associatedtime-varying electric and magnetic fields, respectively, as described infollowing preferred embodiments comprising the preferred embodiments inFIGS. (2) and (6), respectively.); and,

Step 2) from apparatus (2), the beam of electromagnetically neutralizedwave-particle behaving entities (4) is coherently transmitted byapparatus (6) to the target (8). Here, again, during coherenttransmission by apparatus (6) to the target (8), the beam ofelectromagnetically neutralized wave-particle behaving entities (4)comprises waves superimposed out of phase to an extent so to producedestructive interference to an extent, such that the respectiveoscillatory time-varying electromagnetic fields in beam (4) cancel to arespective extent. Wherein, the electromagnetic wave-particle behavingentities in the beam of electromagnetically neutralized wave-particlebehaving entities (4) are electromagnetically neutralized in directproportion to the time-average electric flux density which is eliminatedfrom the beam of electromagnetically neutralized wave-particle behavingentities (4).

In effect, adverse electromagnetic interaction of wave-particle behavingentities in the beam of electromagnetically neutralized wave-particlebehaving entities (4) with electromagnetically functional entitiescomprised in the coherent transmission apparatus (6) is eliminated indirect proportion to the time-average electric flux density which iseliminated from the beam of electromagnetically neutralizedwave-particle behaving entities (4). Hence, an amount of the overalladverse electromagnetic effect of transmitting energy is eliminated to arespective extent. (Note, an electromagnetically functional entity canbe: a) a static electrically charged particle, e.g., a static proton ora static electron which is associated with a non-zero electrostaticfield; b) a propagating electrically charged particle, e.g., apropagating proton or propagating electron comprised in a beamcomprising a non-zero magnitude of time-average electric flux density;or, c) an electromagnetic field quantum comprised in a beam comprising anon-zero magnitude of time-average electric flux density. Also, notethat a given beam of electromagnetically neutralized wave-particlebehaving entities comprises a time-average particle flux density whichcan be determined by the quantization of the time-average electric fluxdensity of a hypothetical beam of wave-particle behaving entities whichis equivalent to the beam of electromagnetically neutralizedwave-particle behaving entities (4) except that the respectivelycomprised waves are totally in phase so to produce complete constructiveinterference such that the associated oscillatory time-varyingelectromagnetic fields totally reinforce. Furthermore, one should beaware of the use of totally electromagnetically neutralizedwave-particle behaving atomic nuclei, e.g., a beam of totallyelectromagnetically neutralized wave-particle behaving protons, for coldnuclear fusion in the preferred embodiment in FIG. (30), before choosinga beam of electromagnetically neutralized wave-particle behavingentities to be applied for any given application.)

FIG. (2) shows a plan side view of a more specific preferred embodimentwhich is applied for the transmission of energy in an effective manner.Steps 1) and 2) comprised in the preferred embodiment in FIG. (1) areapplied in the preferred embodiment in FIG. (2) except that, morespecifically, apparatus (2A) produces a beam of totallyelectromagnetically neutralized wave-particle behaving entities (4A)which is coherently transmitted by coherent transmission apparatus (6A)to the target (8A). In effect, adverse electromagnetic interaction ofthe beam of totally electromagnetically neutralized wave-particlebehaving entities (4A) with electromagnetically functional entitiescomprised in the coherent transmission apparatus (6A) is totallyeliminated in direct proportion to (in agreement with) the totalelimination of the time-average electric flux density from the beam oftotally electromagnetically neutralized wave-particle behaving entities(4A). Hence, the overall adverse electromagnetic effect of transmittingenergy is totally eliminated.

In the preferred embodiment in FIG. (2) coherent transmission processesinvolve potential-energy-type coherent transmission processes whichinvolve a quantum mechanical functional relation between the potentialenergy comprised by coherent transmission apparatus (6A) and the totalenergy comprised by coherently transmitted totally electromagneticallyneutralized wave-particle behaving entities in beam (4A) (refer to thespecific applications for some details of the parameters ofpotential-energy-type coherent transmission media).

(Note, in certain cases, media may exist which does not coherentlytransmit a portion of a given beam of electromagnetically neutralizedwave-particle behaving entities applied. Wherein, such media maycomprise attenuating media which eliminate (e.g., backscatter and/orreflect in a coherent or an incoherent manner) a portion of the totallyelectromagnetically neutralized wave-particle behaving entities from agiven beam of totally electromagnetically neutralized wave-particlebehaving entities applied; and/or comprise incoherently transmittingmedia which incoherently scatter in the forward direction and eliminatean extent of the destructive interference of the waves and respectivecancellation of the associated time-varying electric and magnetic fieldsfrom a given beam of totally electromagnetically neutralizedwave-particle behaving entities applied during transmission to arespective target (refer to FIGS. (15) and (17) for generic descriptionsof apparatus which can incoherently scatter a beam of totallyelectromagnetically neutralized wave-particle behaving entities).

FIG. (3) shows the construction of one version of beam (4A) comprisingthe beam of totally electromagnetically neutralized wave-particlebehaving entities (4B). Beam (4B) is a resultant beam consisting of twocombined coherent beam portions of wave-particle behaving entities (10B)and (12B).

FIG. (3) shows a first coherent beam portion of wave-particle behavingentities (10B) aligned along the direction of propagation (14B) which isparallel to the given (t) axis. The first beam portion of wave-particlebehaving entities (10B) comprises the linearly polarized sinusoidallytime-varying wave component (16B) (of arbitrary wavelength), which islinearly polarized in the (t-y) plane with a particular relative phasealong the (t) axis (as shown aligned along the given (y) axis), and isassociated with a respective linearly polarized sinusoidallytime-varying electric field component (in the t-y plane). The first beamportion of wave-particle behaving entities (10B) also comprises thelinearly polarized sinusoidally time-varying wave component (18B) (of anequivalent arbitrary wavelength), which is linearly polarized in a planewhich is parallel to the given (t-z) plane with an equivalent relativephase along the given (t) axis, and is associated with a respectivelinearly polarized sinusoidally time-varying magnetic field component(in the same t-z plane).

FIG. (3) also shows the second coherent beam portion of wave-particlebehaving entities (12B) aligned along the direction of propagation (20B)which is parallel to the given (t) axis. The second beam portion ofwave-particle behaving entities (12B) comprises the linearly polarizedsinusoidally time-varying wave component (22B) (of an equivalentarbitrary wavelength), which is also linearly polarized in the (t-y)plane with a particular relative phase along the (t) axis (as shownaligned along the given (y) axis), and is associated with a respectivelinearly polarized sinusoidally time-varying electric field component(in the t-y plane). The second beam portion of wave-particle behavingentities (12B) shown also comprises the linearly polarized sinusoidallytime-varying wave component (24B) (of an equivalent arbitrarywavelength), which is also linearly polarized in a plane which isparallel to the (t-z) plane with an equivalent relative phase along thegiven (t) axis, and is associated with a respective linearly polarizedsinusoidally time-varying magnetic field component (in the same t-zplane).

FIG. (3) shows beam (4B) aligned along the direction of propagation(26B), which is parallel to the given (t) axis, consisting of the twocombined coherent beam portions (10B) and (12B). The two beam portions(10B) and (12B) are combined such that the linearly polarizedsinusoidally time-varying wave components (16B) and (22B) aresuperimposed totally out of phase (180 degrees out of phase) so toproduce total destructive interference and the total cancellation ofrespectively associated linearly polarized sinusoidally time-varyingelectric field components, and such that the linearly polarizedsinusoidally time-varying wave components (18B) and (24B) aresuperimposed totally out of phase so to produce total destructiveinterference and the total cancellation of respectively associatedlinearly polarized sinusoidally time-varying magnetic field components.FIG. (3) also shows, along the direction of propagation (26B), which isparallel to the given (t) axis, the superposition resultant of zeromagnitude (28B) (dashed line) associated with an electromagnetic fieldof zero magnitude in beam (4B).

The beam of totally electromagnetically neutralized wave-particlebehaving entities (4B) comprises a respective time-average particle fluxdensity of non-zero magnitude and a respective time-average electricflux density of zero magnitude. Thus, the electromagnetic wave-particlebehaving entities in the beam (4B) are totally electromagneticallyneutralized in direct proportion to (in agreement with) the totalelimination of the time-average electric flux density from the beam oftotally electromagnetically neutralized wave-particle behaving entities(4B).

FIG. (4) shows another version of beam (4A) comprising a beam of totallyelectromagnetically neutralized wave-particle behaving entities which isa resultant beam consisting of two other combined coherent beam portionsof wave-particle behaving entities. The beam of totallyelectromagnetically neutralized wave-particle behaving entities in FIG.(4) is substantially different from the beam of totallyelectromagnetically neutralized wave-particle behaving entities (4B) inFIG. (3) in that the beam of totally electromagnetically neutralizedwave-particle behaving entities in FIG. (4) is pulse modulated (i.e.,on-off keyed) as shown by the two respectively comprised pulses and thespacing between them.

The beam of totally electromagnetically neutralized wave-particlebehaving entities in FIG. (4) comprises a respective time-averageparticle flux density of non-zero magnitude, and comprises a respectivetime-average electric flux density of zero magnitude. Thus, theelectromagnetic wave-particle behaving entities in the beam in FIG. (4)are totally electromagnetically neutralized.

FIG. (5) shows another version of beam (4A) comprising a beam of totallyelectromagnetically neutralized wave-particle behaving entities which isa resultant beam consisting of two other combined coherent beam portionsof wave-particle behaving entities. The beam of totallyelectromagnetically neutralized wave-particle behaving entities in FIG.(5) is substantially different from the beam of totallyelectromagnetically neutralized wave-particle behaving entities in FIG.(4) in that the beam of totally electromagnetically neutralizedwave-particle behaving entities in FIG. (5) is digitally pulse modulated(i.e., digitally on-off keyed) so as to encode data (i.e., here, binarydigital data, 101, from left to right). Wherein, the (1) digits are eachshown by one of the two relatively large pulses which each comprise anon-zero magnitude of particle flux density which is significantlylarger than the particle flux density of the smaller pulse, whichrepresents the digit (0), which is situated between the two relativelylarger pulses.

The beam of totally electromagnetically neutralized wave-particlebehaving entities in FIG. (5) comprises a respective time-averageparticle flux density of non-zero magnitude, and a respectivetime-average electric flux density of zero magnitude. Thus, theelectromagnetic wave-particle behaving entities in the beam in FIG. (5)are totally electromagnetically neutralized.

FIG. (6) shows a plan side view of another more specific preferredembodiment which is applied for the transmission of energy in aneffective manner. Steps 1) and 2) comprised in the preferred embodimentin FIG. (1) are also applied in the preferred embodiment in FIG. (6)except that the beam of electromagnetically neutralized wave-particlebehaving entities which is applied in the preferred embodiment in FIG.(6), more specifically, comprises apparatus (2C) which produces a beamof partly electromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities (4C) which is coherentlytransmitted by the coherent transmission apparatus (6C) to the target(8C). In effect, adverse electromagnetic interaction of the beam ofpartly electromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities (4C) with electromagneticallyfunctional entities comprised in the coherent transmission apparatus(6C) is eliminated in direct proportion to the time-average electricflux density which is eliminated from the beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities (4C). Hence, the overalladverse electromagnetic effect of transmitting energy is eliminated to aproportional extent. (Note, conversely, the beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities (4C) can electromagneticallyinteract with electromagnetically functional entities comprised in thecoherent transmission apparatus (6C) in direct proportion to thetime-average electric flux density which remains in the beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities (4C). Wherein, an extent ofthe adverse electromagnetic effects of transmitting energy can exist toa respective extent.)

In the preferred embodiment in FIG. (6) the beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities (4C) is coherentlytransmitted by coherent transmission processes which involvepotential-energy-type coherent transmission processes which involve aquantum mechanical functional relation between the potential energycomprised by the coherent transmission apparatus (6C) and the totalenergy comprised by coherently transmitted partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities; and coherent transmission processes can also involveelectromagnetic-type coherent transmission processes which involveelectromagnetic interaction (refer to the specific applications for somedetails of the parameters of electromagnetic-type coherent transmissionmedia).

(Note, in certain cases, media may exist which does not coherentlytransmit a portion of a given beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities applied. Wherein, such media may comprise attenuatingmedia which eliminate (e.g., backscatter and/or reflect in a coherent oran incoherent manner) a portion of the partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities from a given beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities applied; and/or comprise incoherently transmittingmedia which incoherently scatter in the forward direction and eliminatean extent of the destructive interference of waves and respectivecancellation of associated time-varying electric and magnetic fieldsfrom a given beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities appliedduring transmission (refer, for example, to FIGS. (15), (16), and (17)for generic descriptions of apparatus which can incoherently scatter abeam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities).)

FIG. (7) shows the construction of one version of beam (4C) comprising abeam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities (4E)which is a resultant beam consisting of two combined coherent beamportions (10E) and (12E). The beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities (4E) in FIG. (7) is produced differently from the beamof totally electromagnetically neutralized wave-particle behavingentities (4B) in FIG. (3) by changing the relative phase relationbetween the linearly polarized sinusoidally time-varying electromagneticwave components comprised by the respectively comprised coherent beamportions comprised in beam (4E).

FIG. (7) shows the first coherent beam portion of wave-particle behavingentities (10E) aligned along the direction of propagation (14E) which isparallel to the given (t) axis. The first beam portion of wave-particlebehaving entities (10E) comprises the linearly polarized sinusoidallytime-varying wave component (16E) (of arbitrary wavelength), which islinearly polarized in the (t-y) plane with a particular relative phasealong the (t) axis (as shown aligned along the given (y) axis), and isassociated with a respective linearly polarized sinusoidallytime-varying electric field component (in the t-y plane). The first beamportion of wave-particle behaving entities (10E) also comprises thelinearly polarized sinusoidally time-varying wave component (18E) (of anequivalent arbitrary wavelength), which is linearly polarized in a planewhich is parallel to the (t-z) plane with an equivalent relative phasealong the given (t) axis, and is associated with a respective linearlypolarized sinusoidally time-varying magnetic field component (in thesame t-z plane).

FIG. (7) also shows the second coherent beam portion of wave-particlebehaving entities (12E) aligned along the direction of propagation (20E)which is parallel to the given (t) axis. The second beam portion ofwave-particle behaving entities (12E) comprises the linearly polarizedsinusoidally time-varying wave component (22E) (of an equivalentarbitrary wavelength), which is linearly polarized in the (t-y) planewith a particular relative phase along the (t) axis (as shown alignedalong the given (y) axis), and is associated with a respective linearlypolarized sinusoidally time-varying electric field component (in the t-yplane). The second beam portion of wave-particle behaving entities (12E)also comprises the linearly polarized sinusoidally time-varying wavecomponent (24E) (of an equivalent arbitrary wavelength), which islinearly polarized in a plane which is parallel to the (t-z) plane withan equivalent relative phase along the given (t) axis, and is associatedwith a respective linearly polarized sinusoidally time-varying magneticfield component (in the same t-z plane).

FIG. (7) shows beam (4E) aligned along the direction of propagation(26E), which is parallel to the given (t) axis. Here, beam (4E) is theresult of the two combined coherent beam portions of wave-particlebehaving entities (10E) and (12E). The beam portions (10E) and (12E) arecombined such that the linearly polarized sinusoidally time-varying wavecomponent (16E) and (22E) are superimposed partly out of phase (somedegree out of phase between zero degrees out of phase and 180 degreesout of phase) so to produce partial destructive interference and partialcancellation of the respectively associated linearly polarizedsinusoidally time-varying electric field components, and such that thelinearly polarized sinusoidally time-varying wave components (18E) and(24E) are superimposed partly out of phase (the same degree out of phasewhich is between zero degrees out of phase and 180 degrees out of phase)so to produce partial destructive interference to an extent and partialcancellation of the respectively associated linearly polarizedsinusoidally time-varying magnetic field components to a respectiveextent.

The beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities (4E)comprises the superposition resultant linearly polarized sinusoidallytime-varying wave (28E) comprising the linearly polarized sinusoidallytime-varying superposition resultant wave component (30E) which is inthe (t-y) plane) and is associated with a resultant linearly polarizedsinusoidally time-varying electric field (in the t-y plane), and thesuperposition resultant linearly polarized sinusoidally time-varyingwave (28E) comprises the linearly polarized sinusoidally time-varyingsuperposition resultant wave component (32E) which is in a planeparallel to the (t-z) plane and is associated with a resultant linearlypolarized sinusoidally time-varying magnetic field (in the same t-zplane).

The beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities (4E)comprises a respective time-average particle flux density of non-zeromagnitude, and a respective time-average electric flux density ofnon-zero magnitude. Wherein, the electromagnetic wave-particle behavingentities in the beam of partly electromagnetically neutralized andpartly electromagnetically functional wave-particle behaving entities(4E) are electromagnetically neutralized in direct proportion to thetime-average electric flux density eliminated from beam (4E), and areelectromagnetically functional in direct proportion to the time-averageelectric flux density which remains in the beam (4E). (Note, thetime-average electric flux density of a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities has a magnitude which isbetween zero and a maximum magnitude which would be produced by ahypothetical beam of electromagnetic wave-particle behaving entities (ofequivalent type and wavelength) which comprises an equivalent magnitudeof time-average particle flux density and which comprises waves whichare superimposed totally in phase to produce total constructiveinterference, such that the respective oscillatory time-varyingelectromagnetic fields in the hypothetical beam totally reinforce.)

FIG. (8) shows another version of beam (4C) comprising a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities which is a resultant beamconsisting of two other combined coherent beam portions. The beam ofpartly electromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities in FIG. (8) is substantiallydifferent from the beam of partly electromagnetically neutralized andpartly electromagnetically functional wave-particle behaving entities(4E) in FIG. (7) in that the beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities in FIG. (8) is pulse modulated (i.e., on-off keyed) asshown by the two respectively comprised pulses and the spacing betweenthem.

The beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities in FIG.(8) comprises a respective time-average particle flux density ofnon-zero magnitude, and a respective time-average electric flux densityof non-zero magnitude. Wherein, the electromagnetic wave-particlebehaving entities in the beam of partly electromagnetically neutralizedand partly electromagnetically functional wave-particle behavingentities in FIG. (8) are electromagnetically neutralized in directproportion to the time-average electric flux density eliminated frombeam in FIG. (8), and are electromagnetically functional in directproportion to the time-average electric flux density which remains inthe beam in FIG. (8).

FIG. (9) shows another version of beam (4C) comprising a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities which is a resultant beamconsisting of two other combined coherent beam portions. The beam ofpartly electromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities in FIG. (9) is substantiallydifferent from the beam of partly electromagnetically neutralized andpartly electromagnetically functional wave-particle behaving entities(4E) in FIG. (8) in that the beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities in FIG. (9) is digitally pulse modulated (i.e.,digitally on-off keyed) so as to encode data (i.e., here, binary digitaldata, 101, from left to right). Wherein, the (1) digits are each shownby one of the two relatively large pulses which each comprise a non-zeromagnitude of particle flux density which is significantly larger thanthe particle flux density of the smaller pulse, which represents thedigit (0), which is situated between the two relatively larger pulses.

The beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities comprisesa respective time-average particle flux density of non-zero magnitude,and a respective time-average electric flux density of non-zeromagnitude. Wherein, the electromagnetic wave-particle behaving entitiesin the beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities in FIG.(9) are electromagnetically neutralized in direct proportion to thetime-average electric flux density eliminated from beam in FIG. (9), andare electromagnetically functional in direct proportion to thetime-average electric flux density which remains in the beam in FIG.(9).

FIG. (10) shows a preferred embodiment which is applied for thetransmission and subsequent utilization of momentum in an effectivemanner. Steps 1) and 2) comprised in the preferred embodiment in FIG.(2) or (6) can be applied in the preferred embodiment in FIG. (10) withthe addition of a step.

In the preferred embodiment in FIG. (10), apparatus produces a beam ofelectromagnetically neutralized wave-particle behaving entitiescomprising a least one discontinuity of momentum (such as a continuousbeam of electromagnetically neutralized wave-particle behaving entitieswith a discontinuous leading and/or a discontinuous falling edge; or apulse modulated beam of electromagnetically neutralized wave-particlebehaving entities as shown in FIG. (4), (5), (8), or (9)). Then, therespective beam of electromagnetically neutralized wave-particlebehaving entities is coherently transmitted by coherent transmissionapparatus to a target (block comprising the dashed line format) whichcomprises a momentum-type utilizing apparatus (e.g., a pressuretransducer), such that adverse electromagnetic interaction of therespective beam of electromagnetically neutralized wave-particlebehaving entities with electromagnetically functional entities comprisedin the coherent transmission apparatus is eliminated to an extent.Wherein, adverse electromagnetic effects of transmitting energy for therespective application are eliminated to an extent.

In addition, the preferred embodiment in FIG. (10) comprises thefollowing step:

Step 3) the utilization of transmitted momentum comprised by thecoherently transmitted beam of electromagnetically neutralizedwave-particle behaving entities by the momentum-type utilizingapparatus. In this case, the coherently transmitted beam ofelectromagnetically neutralized wave-particle behaving entities impartsmomentum upon the momentum-type utilizing apparatus which utilizes theapplied momentum to produce the result of the respective preferredembodiment (e.g., the coherently transmitted beam of electromagneticallyneutralized wave-particle behaving entities can impart momentum to,i.e., apply pressure upon, a pressure transducer which can utilizemomentum by way of Newton's second law of physics in which, for example,momentum would be applied to the pressure transducer by a momentumvector which is equal in magnitude and opposite in direction to thechange of the momentum vector of the respectively reflected beam ofelectromagnetically neutralized wave-particle behaving entities).

FIG. (11) shows a preferred embodiment which is applied for thetransmission and subsequent utilization of energy in an effectivemanner. Steps 1) and 2) comprised in the preferred embodiment in FIG.(6) are applied in the preferred embodiment in FIG. (11) with theaddition of a step.

In the preferred embodiment in FIG. (11), apparatus produces a beam ofpartly electromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities which is coherentlytransmitted by coherent transmission apparatus to a target (blockcomprising the dashed line format), such that adverse electromagneticinteraction of the beam of partly electromagnetically neutralized andpartly electromagnetically functional wave-particle behaving entitieswith electromagnetically functional entities comprised in the coherenttransmission apparatus is eliminated to an extent. Wherein, the adverseelectromagnetic effects of transmitting energy for the respectiveapplication are eliminated to an extent.

Wherein, in addition, the preferred embodiment in FIG. (11) comprisesthe following step:

Step 3) the utilization of coherently transmitted partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities by electromagnetic-typeutilizing apparatus comprised in the target. In this case, thecoherently transmitted beam of partly electromagnetically neutralizedand partly electromagnetically functional wave-particle behavingentities applies (and/or inputs) partly electromagnetically neutralizedand partly electromagnetically functional wave-particle behavingentities upon (or into) the electromagnetic-type utilizing apparatuswhich comprises electromagnetically functional entities. Wherein,electromagnetically functional entities comprised in theelectromagnetic-type utilizing apparatus utilize transmitted partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities by way of electromagneticinteraction to produce the result of the respective preferredembodiment.

FIG. (12) shows another preferred embodiment which is applied for thetransmission and subsequent utilization of energy in an effectivemanner. Steps 1) and 2) comprised in the preferred embodiment in FIG.(6) are applied in the preferred embodiment in FIG. (12) with theaddition of two steps.

In the preferred embodiment in FIG. (12), apparatus produces a beam ofpartly electromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities by combining, for example,two linearly polarized sinusoidally time-varying coherent beams ofwave-particle behaving entities which each comprises a plane ofpolarization with a slightly different angle of rotation, or also aresuperimposed partly out of phase. Wherein, the beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities comprises coherent waveswhich destructively interfere to an extent and associated time-varyingelectric and magnetic fields which partly cancel, respectively, to anextent.

Then, the beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities iscoherently transmitted by coherent transmission apparatus to a target(block comprising the dashed line format), such that adverseelectromagnetic interaction of the beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities with electromagnetically functional entities comprisedin the coherent transmission apparatus is eliminated to an extent.Wherein, the adverse electromagnetic effects of transmitting energy forthe respective application are eliminated to an extent. Here, morespecifically, the target comprises a polarizer and anelectromagnetic-type utilizing apparatus comprising electromagneticallyfunctional entities.

Then, the preferred embodiment in FIG. (12) comprises the followingadditional steps:

Step 3) in which, as examples:

a) one of the two linearly polarized coherent beam portions ofwave-particle behaving entities comprised in the coherently transmittedbeam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities can bereflected along Brewster's angle by a polarizer comprised in the targetin order to separate the one linearly polarized coherent beam portion ofwave-particle behaving entities from the other linearly polarizedcoherent beam portion of wave-particle behaving entities comprised inthe coherently transmitted beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities, such that destructive interference of waves andrespective cancellation of associated time-varying electric and magneticfields in the coherently transmitted beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities are respectively eliminated. Wherein, in effect, twolinearly polarized beams of electromagnetically functional wave-particlebehaving entities are produced. (Here, apparatus can produce a beam ofpartly electromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities with one or more otherlinearly polarized coherent beam portions of wave-particle behavingentities added, which, along with all the other linearly polarizedcoherent beam portions of wave-particle behaving entities, would betransmitted to a target comprising additional polarizers which wouldseparate each of the linearly polarized coherent beam portions forsubsequent utilization); or,

b) one of the two linearly polarized coherent beam portions ofwave-particle behaving entities comprised in the coherently transmittedbeam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities can befiltered out of the coherently transmitted beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities by a polarizing filter in thetarget, such that destructive interference of waves and respectivecancellation of associated time-varying electric and magnetic fields inthe coherently transmitted beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities is eliminated. Wherein, only one linearly polarizedcoherent beam of electromagnetically functional wave-particle behavingentities would remain. In any such case, polarization involveselectromagnetic interaction. (Note, a beam of electromagneticallyfunctional wave-particle behaving entities can comprise a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities or a beam of totallyelectromagnetically functional wave-particle behaving entitiescomprising wave-particle behaving entities comprising waves whichtotally constructively interfere with associated electromagnetic fieldswhich totally reinforce.)

Also, step 3) comprises the transmission of the linearly polarized beam(or beams) of electromagnetically functional wave-particle behavingentities by transmission apparatus comprised by the polarizer comprisedin the target (or also comprised in the electromagnetic-type utilizingapparatus) to electromagnetic-type utilizing apparatus; and, then,

Step 4) the utilization of the transmitted linearly polarized beam (orbeams) of electromagnetically functional wave-particle behaving entitiesby electromagnet-type utilizing apparatus comprising electromagneticallyfunctional entities by way of electromagnetic interaction to produce theresult of the respective preferred embodiment.

FIG. (13) is another preferred embodiment which is applied for thetransmission and subsequent utilization of energy in an effectivemanner. Steps 1) and 2) comprised in the preferred embodiment in FIG.(2) or (6) can be applied in the preferred embodiment in FIG. (13) withthe addition of two steps.

In the preferred embodiment in FIG. (13), apparatus produces a beam ofelectromagnetically neutralized wave-particle behaving entities which iscoherently transmitted by coherent transmission apparatus to a target(block comprising the dashed line format), such that adverseelectromagnetic interaction of the beam of electromagneticallyneutralized wave-particle behaving entities with electromagneticallyfunctional entities comprised in the coherent transmission apparatus iseliminated to an extent. Wherein, the adverse electromagnetic effects oftransmitting energy for the respective application are eliminated to anextent. Here, more specifically, the target comprises apotential-energy-type incoherently scattering and transmittingapparatus, and electromagnetic-type utilizing apparatus.

Wherein, in addition, the preferred embodiment in FIG. (13) comprisesthe following steps:

Step 3) the incoherent scattering of the coherently transmitted beam ofelectromagnetically neutralized wave-particle behaving entities to anextent by the potential-energy-type incoherently scattering apparatuscomprised by a potential-energy-type incoherently scattering andtransmitting apparatus comprised in the target so to produce a beam ofelectromagnetically functional wave-particle behaving entities in thepotential-energy-type incoherently scattering and transmittingapparatus. Wherein, the beam of electromagnetically functionalwave-particle behaving entities produced by potential-energy-typeincoherent scattering comprises electromagnetically functionalwave-particle behaving entities comprising randomly distributed waveswith random relative phase relations which neither superimpose norinterfere, such that associated electric and magnetic field intensitiesrespectively add, and thus produce a non-zero magnitude of time-averageelectric flux density in the respective potential-energy-typeincoherently scattering and transmitting apparatus (or also the beam ofelectromagnetically functional wave-particle behaving entities cancomprise any remaining portion of a beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities which is not incoherently scattered if a beam ofpartly electromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities is applied). (Note, anelectromagnetically functional wave-particle behaving entity is awave-particle behaving entity which is associated with non-zerotime-varying electromagnetic field, which produce a non-zero timeaverage electric flux density, such that an electromagneticallyfunctional wave-particle behaving entity is either totallyelectromagnetically functional if comprised in an incoherent beam ofwave-particle behaving entities or comprised in a beam of totallyelectromagnetically functional wave-particle behaving entities; andconsidered partly electromagnetically functional if comprised in a beamof partly electromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities.)

In this case, potential-energy-type incoherently scattering apparatuscomprises an irregularly ordered distribution of particles which eachcomprise: a) potential energy which changes significantly relative tothe potential energy of its respective surroundings and the total energycomprised by each of the respective incoherently scattered wave-particlebehaving entities; and b) a size and spacing which are each comparableto, or significantly larger than, the wavelength of the waves comprisedby respective wave-particle behaving entities which are incoherentlyscattered from the beam of electromagnetically neutralized wave-particlebehaving entities. Wherein, potential-energy-type incoherent scatteringprocesses (e.g., irregular reflections and/or irregular refractions)involve a quantum mechanical functional relation between the potentialenergy comprised by potential-energy-type incoherently scatteringapparatus and the total energy comprised by the respective incoherentlyscattered wave-particle behaving entities.

Also, in step 3), an extent of the beam of electromagneticallyfunctional wave-particle behaving entities produced bypotential-energy-type incoherent scattering (or also an extent of anyremaining portion of a beam of partly electromagnetically neutralizedand partly electromagnetically functional wave-particle behavingentities which is not incoherently scattered if a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities is applied) is transmitted bytransmission apparatus comprised in the potential-energy-typeincoherently scattering and transmitting apparatus (or also comprised inthe utilizing apparatus) to electromagnetic-type utilizing apparatuscomprised in the target. (Note, though transmitting apparatus comprisedin potential-energy-type incoherently scattering and transmittingapparatus generally includes the potential-energy-type incoherentlyscattering apparatus, other transmitting apparatus can exist inpotential-energy-type incoherently scattering apparatus and/or inelectromagnetic-type utilizing apparatus in this step, and all suchtransmission apparatus would require any parameters with respectivevalues which would effectively transmit the respectiveelectromagnetically functional wave-particle behaving entities applied);and, then,

Step 4) Utilization of an extent of the transmitted beam ofelectromagnetically functional wave-particle behaving entities by way ofelectromagnetic interaction by the electromagnetic-type utilizingapparatus comprising electromagnetically function entities to producethe result of the respective preferred embodiment (i.e., an extent ofthe transmitted electromagnetically functional wave-particle behavingentities produced by potential-energy-type incoherent scattering or alsoan extent of any transmitted remaining portion of a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities which was not incoherentlyscattered, if a beam of partly electromagnetically neutralized andpartly electromagnetically functional wave-particle behaving entities isapplied, are utilized by way of electromagnetic interaction byelectromagnetic-type utilizing apparatus comprising electromagneticallyfunctional entities to produce the result of the respective preferredembodiment).

FIG. (14) shows another preferred embodiment which is applied for thetransmission and subsequent utilization of energy in an effectivemanner. Steps 1) and 2) comprised in the preferred embodiment in FIG.(6) are applied in the preferred embodiment in FIG. (14) with theaddition of two steps.

Wherein, in the preferred embodiment in FIG. (14), apparatus produces abeam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities which iscoherently transmitted by coherent transmission apparatus to a target(block comprising the dashed line format), such that adverseelectromagnetic interaction of the beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities with electromagnetically functional entities comprisedin the coherent transmission apparatus is eliminated to an extent.Wherein, the adverse electromagnetic effects of transmitting energy forthe respective application are eliminated to an extent. Here, morespecifically, the target comprises electromagnetic-type incoherentlyscattering and transmitting apparatus and an electromagnetic-typeutilizing apparatus comprising electromagnetically functional entities.

Then, the preferred embodiment in FIG. (14) comprises the followingadditional steps:

Step 3) the incoherent scattering of the coherently transmitted beam ofpartly electromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities to an extent byelectromagnetic-type incoherently scattering apparatus comprisingelectromagnetically functional entities comprised in anelectromagnetic-type incoherently scattering and transmitting apparatuscomprised in the target. Wherein, the incoherently scattered beam ofelectromagnetically functional wave-particle behaving entities in theelectromagnetic-type incoherently scattering and transmitting apparatuscomprises electromagnetically functional wave-particle behaving entitiescomprising randomly distributed waves with random relative phaserelations which neither superimpose nor interfere, such that associatedelectric and magnetic field intensities respectively add, and thusproduce a non-zero magnitude of time-average electric flux density inthe respective electromagnetic-type incoherently scattering andtransmitting apparatus (or also the beam of electromagneticallyfunctional wave-particle behaving entities can comprise any remainingportion of the beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities which isnot incoherently scattered). (Note, an electromagnetically functionalwave-particle behaving entity is a wave-particle behaving entity whichis associated with non-zero time-varying electric and magnetic fields,which produce a non-zero time average electric flux density, and such anelectromagnetically functional wave-particle behaving entity is eithertotally electromagnetically functional or partly electromagneticallyneutralized and partly electromagnetically functional according to theextent of destructive interference of waves and respective cancellationof associated time-varying electric and magnetic fields in the beamwhich comprises the respective electromagnetically functionalwave-particle behaving entity.)

In this case, electromagnetic-type incoherently scattering apparatuscomprises an irregularly ordered distribution of electromagneticallyfunctional entities (e.g., atoms and molecules) which each comprisespacing which is comparable to, or significantly larger than, thewavelength of the waves comprised by the respective incoherentlyscattered electromagnetically functional wave-particle behavingentities. Wherein, electromagnetic-type incoherent scattering processes(e.g., incoherent reradiation scattering) involve electromagneticinteraction.

Also, in step 3), an extent of the beam of electromagneticallyfunctional wave-particle behaving entities produced byelectromagnetic-type incoherent scattering (or also an extent of anyremaining portion of the beam of partly electromagnetically neutralizedand partly electromagnetically functional wave-particle behavingentities which is not incoherently scattered) is transmitted bytransmission apparatus to the electromagnetic-type utilizing apparatuscomprised in the target). (Note, though transmitting apparatus comprisedin electromagnetic-type incoherently scattering and transmittingapparatus generally includes the electromagnetic-type incoherentlyscattering apparatus, other transmitting apparatus can exist inelectromagnetic-type incoherently scattering and transmitting apparatusand/or in the electromagnetic-type utilizing apparatus in this step, andall such transmission apparatus would require any parameters withrespective values which would effectively transmit the respectiveelectromagnetically functional wave-particle behaving entities applied);and, then,

Step 4) the utilization of an extent of the beam of transmittedelectromagnetically functional wave-particle behaving entities by way ofelectromagnetic interaction by electromagnetic-type utilizing apparatuscomprising electromagnetically functional entities to produce the resultof the respective preferred embodiment (i.e., an extent of thetransmitted electromagnetically functional wave-particle behavingentities produced by electromagnetic-type incoherent scattering or alsoan extent of any transmitted remaining portion of the beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities applied are utilized by wayof electromagnetic interaction by electromagnetic-type utilizingapparatus to produce the result of the respective preferred embodiment).In this case, electromagnetic-type utilizing apparatus compriseselectromagnetically functional entities, and the utilization processinvolves electromagnetic interaction.

FIG. (15) shows another preferred embodiment which is applied for thetransmission and subsequent utilization of energy in an effectivemanner. Steps 1), 2), 3), and 4) comprised in the preferred embodimentin FIG. (13) are applied in the preferred embodiment in FIG. (15)except, in addition, an electromagnetic-type incoherently scattering andtransmitting apparatus is positioned between a potential-energy-typeincoherently scattering and transmitting apparatus, and anelectromagnetic-type utilizing apparatus; step 3) is considered step3a), and, in addition, a step 3b) is inserted between what is now step3a) and step 4).

Wherein, in the preferred embodiment in FIG. (15), apparatus produces abeam of electromagnetically neutralized wave-particle behaving entitieswhich is coherently transmitted by coherent transmission apparatus to atarget (block comprising the dashed line format), such that adverseelectromagnetic interaction of the beam of electromagneticallyneutralized wave-particle behaving entities with electromagneticallyfunctional entities comprised in the coherent transmission apparatus iseliminated to an extent. Wherein, the adverse electromagnetic effects oftransmitting energy for the respective application are eliminated to anextent. Here, more specifically, the target comprises apotential-energy-type incoherently scattering and transmittingapparatus, electromagnetic-type incoherently scattering and transmittingapparatus, and electromagnetic-type utilizing apparatus.

Then, in step 3a), the coherently transmitted beam ofelectromagnetically neutralized wave-particle behaving entities isincoherently scattered to an extent by potential-energy-type incoherentscattering so to produce a beam of electromagnetically functionalwave-particle behaving entities (which comprises a non-zero time-averageelectric flux density) in the potential-energy-type incoherentlyscattering and transmitting apparatus (i.e., a beam ofelectromagnetically functional wave-particle behaving entities isproduced comprising electromagnetically functional wave-particlebehaving entities produced by potential-energy-type incoherentscattering or also comprising any remaining portion of a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities which is not incoherentlyscattered if a beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities isapplied). Also, in step 3a), transmission apparatus comprised in thepotential-energy-type incoherently scattering and transmitting apparatus(or also the electromagnetic-type utilizing apparatus) transmits anextent of the beam of electromagnetically functional wave-particlebehaving entities produced by potential-energy-type incoherentscattering (or also transmits any remaining portion of a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities which is not incoherentlyscattered if a beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities isapplied) to electromagnetic-type incoherently scattering andtransmitting apparatus.

Then, in addition, between step 3a) and step 4), the preferredembodiment in FIG. (15) comprises:

Step 3b) the beam of electromagnetically functional wave-particlebehaving entities is incoherently scattered to an extent byelectromagnetic-type incoherently scattering apparatus comprisingelectromagnetically functional entities so to produce an effectivelydifferent combined beam of electromagnetically functional wave-particlebehaving entities in the electromagnetic-type incoherently scatteringapparatus (i.e., electromagnetic-type incoherently scattering apparatusincoherently scatters an extent of the transmitted electromagneticallyfunctional wave-particle behaving entities produced bypotential-energy-type incoherent scattering or also incoherentlyscatters an extent of any transmitted remaining portion of a beam ofpartly electromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities which is not incoherentlyscattered, if a beam of partly electromagnetically neutralized andpartly electromagnetically functional wave-particle behaving entities isapplied, to produce an effectively different beam of electromagneticallyfunctional wave-particle behaving entities comprisingelectromagnetically functional wave-particle behaving entities producedby combined potential-energy-type and electromagnetic-type incoherentscattering or also comprising any transmitted remaining portion of abeam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities which isnot incoherently scattered if a beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities is applied).

Wherein, the combined beam of electromagnetically functionalwave-particle behaving entities in the electromagnetic-type incoherentlyscattering and transmitting apparatus comprises electromagneticallyfunctional wave-particle behaving entities comprising randomlydistributed waves with random relative phase relations which neithersuperimpose nor interfere, such that associated electric and magneticfield intensities respectively add, and thus electromagnetic-typeincoherently scattering apparatus, along with potential-energy-typeincoherently scattering apparatus, produce a beam of electromagneticallyfunctional wave-particle behaving entities (which comprises a non-zeromagnitude of time-average electric flux density) in the respectiveelectromagnetic-type incoherently scattering and transmitting apparatus.Also, step 3b) comprises the transmission of an extent of the combinedbeam of electromagnetically functional wave-particle behaving entitiesby transmission apparatus comprised in the electromagnetic-typeincoherently scattering and transmitting apparatus (or also comprised inthe electromagnetic-type utilizing apparatus) to electromagnetic-typeutilizing apparatus (i.e., electromagnetically functional wave-particlebehaving entities produced by combined potential-energy-type andelectromagnetic-type incoherent scattering or also any remaining portionof a beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities which isnot incoherently scattered, if a beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities is applied, are transmitted by transmitting apparatusto the electromagnetic-type utilizing apparatus).

Wherein, subsequently, an extent of the transmitted beam ofelectromagnetically functional wave-particle behaving entities isutilized by electromagnetic interaction by electromagnetic-typeutilizing apparatus comprising electromagnetically functional entitiesto produce the result of the respective preferred embodiment of thepresent invention (i.e., an extent of the transmittedelectromagnetically functional wave-particle behaving entities producedby combined potential-energy-type and electromagnetic-type incoherentscattering or also an extent of any transmitted remaining portion of abeam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities which isnot incoherently scattered, if a beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities is applied, are utilized by way of electromagneticinteraction by electromagnetic-type utilizing apparatus to produce theresult of the respective preferred embodiment).

FIG. (16) shows another preferred embodiment which is applied for thetransmission and subsequent utilization of energy in an effectivemanner. Steps 1), 2), 3), and 4) comprised in the preferred embodimentin FIG. (14) are applied in the preferred embodiment in FIG. (16) excepta potential-energy-type incoherently scattering and transmittingapparatus is positioned between electromagnetic-type incoherentlyscattering and transmitting apparatus, and electromagnetic-typeutilizing apparatus; step 3) is considered step 3a), and, in addition, astep 3b) is inserted between what is now step 3a) and step 4).

In the preferred embodiment in FIG. (16), apparatus produces a beam ofpartly electromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities which is coherentlytransmitted by coherent transmission apparatus to a target (blockcomprising the dashed line format), such that adverse electromagneticinteraction of the beam of partly electromagnetically neutralized andpartly electromagnetically functional wave-particle behaving entitieswith electromagnetically functional entities comprised in the coherenttransmission apparatus is eliminated to an extent. Wherein, the adverseelectromagnetic effects of transmitting energy for the respectiveapplication are eliminated to an extent. Here, more specifically, thetarget comprises an electromagnetic-type incoherently scattering andtransmitting apparatus, a potential-energy-type incoherently scatteringand transmitting apparatus, and an electromagnetic-type utilizingapparatus.

Wherein, then, in step 3a) the beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities is incoherently scattered to an extent byelectromagnetic-type incoherently scattering apparatus comprised in thetarget so to produce a beam of electromagnetically functionalwave-particle behaving entities (comprising a non-zero time-averageelectric flux density) in the electromagnetic-type incoherentlyscattering and transmitting apparatus (i.e., a beam ofelectromagnetically functional wave-particle behaving entities isproduced comprising electromagnetically functional wave-particlebehaving entities produced by electromagnetic-type incoherent scatteringor also any remaining portion of the beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities which is not incoherently scattered).

An extent of such a beam of electromagnetically functional wave-particlebehaving entities produced is transmitted by transmission apparatuscomprised in the electromagnetic-type incoherently scattering andtransmitting apparatus (or also the electromagnetic-type utilizingapparatus) to the potential-energy-type incoherently scattering andtransmitting apparatus comprised in the target (i.e.,electromagnetically functional wave-particle behaving entities producedby electromagnetic-type incoherent scattering or also any remainingportion of the beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities which isnot incoherently scattered are transmitted by transmission apparatus tothe potential-energy-type incoherently scattering and transmittingapparatus comprised in the target).

Then, in step 3b), the potential-energy-type incoherently scatteringapparatus comprised in the target incoherently scatters an extent of anyremaining portion of the coherently transmitted beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities (and the beam ofelectromagnetically functional wave-particle behaving entities producedby electromagnetic-type incoherent scattering) so to produce aneffectively different beam of electromagnetically functionalwave-particle behaving entities (which comprises a non-zero magnitude oftime-average electric flux density) in the potential-energy-typeincoherently scattering and transmitting apparatus. The effectivelydifferent beam of electromagnetically functional wave-particle behavingentities produced herein comprises electromagnetically functionalwave-particle behaving entities produced by combinedelectromagnetic-type incoherent scattering and potential-energy-typeincoherent scattering or also comprises any remaining portion of thebeam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities appliedwhich is still not incoherently scattered.

Wherein, such a beam of electromagnetically functional wave-particlebehaving entities produced comprises electromagnetically functionalwave-particle behaving entities comprising randomly distributed waveswith random relative phase relations which neither superimpose norinterfere, such that associated electric and magnetic fieldsrespectively add, and thus electromagnetic-type incoherent scatteringand potential-energy-type incoherent scattering combine to produce abeam of electromagnetically functional wave-particle behaving entities(which comprises a non-zero magnitude of time-average electric fluxdensity) in the respective potential-energy-type incoherently scatteringand transmitting apparatus. In this case, potential-energy-typeincoherently scattering apparatus comprises parameters and followsrespective potential-energy-type incoherent scattering processes asdescribed in the preferred embodiment in FIG. (13).

Also, step 3b) comprises the transmission of an extent of the combinedbeam of electromagnetically functional wave-particle behaving entitiesby transmission apparatus comprised in the potential-energy-typeincoherently scattering and transmitting apparatus (or also theelectromagnetic-type utilizing apparatus) to electromagnetic-typeutilizing apparatus comprised in the target (i.e., electromagneticallyfunctional wave-particle behaving entities produced by combinedelectromagnetic-type incoherent scattering and potential-energy-typeincoherent scattering or also any remaining portion of the beam ofpartly electromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities applied which was notincoherently scattered are transmitted by transmission apparatus to theelectromagnetic-type utilizing apparatus comprised in the target).

Wherein, subsequently, an extent of the transmitted beam ofelectromagnetically functional wave-particle behaving entities isutilized by way of electromagnetic interaction by electromagnetic-typeutilizing apparatus comprising electromagnetically functional entitiesto produce the result of the respective preferred embodiment of thepresent invention (i.e., an extent of the transmittedelectromagnetically functional wave-particle behaving entities producedby combined electromagnetic-type and potential-energy-type incoherentscattering, or also an extent of any transmitted remaining portion ofthe beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities which wasnot incoherently scattered, are utilized by way of electromagneticinteraction by electromagnetic-type utilizing apparatus to produce theresult of the respective preferred embodiment of the present invention).

FIG. (17) shows a somewhat generic preferred embodiment which is appliedfor the transmission and subsequent utilization of energy in aneffective manner. The preferred embodiment in FIG. (17) is a conditionalpreferred embodiment which would apply certain steps as applied in theaforedescribed preferred embodiments dependent upon which type of beamof electromagnetically neutralized wave-particle behaving entities isapplied; combines potential-energy-type and electromagnetic-typeincoherently scattering and transmitting apparatus into one apparatus(when applied together); and combines the steps applied by therespectively combined apparatus.

Wherein, if a beam of totally electromagnetically neutralizedwave-particle behaving entities were applied, then the preferredembodiment in FIG. (17) can apply steps comprising potential-energy-typeincoherent scattering and transmission, or also electromagnetic-typeincoherent scattering and transmission, and subsequently a step for theutilization of electromagnetically functional wave-particle behavingentities as applied in the preferred embodiments in FIG. (13) or also(14). Wherein, the preferred embodiment in FIG. (17) would comprise asingle incoherently scattering and transmitting apparatus which wouldcomprise potential-energy-type incoherently scattering and transmittingapparatus or also electromagnetic-type incoherently scattering andtransmitting apparatus.

However, if a beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities wereapplied, then the preferred embodiment in FIG. (17) can apply stepscomprising electromagnetic-type incoherent scattering and transmissionand/or potential-energy-type incoherent scattering and transmission, andsubsequently a step for the utilization of electromagneticallyfunctional wave-particle behaving entities as applied in the preferredembodiments in FIGS. (13) and/or (14). However, in this case, thepreferred embodiment in FIG. (17) would comprise a single incoherentlyscattering and transmitting apparatus which would compriseelectromagnetic-type incoherently scattering and transmitting apparatusand/or potential-energy-type incoherently scattering and transmittingapparatus.

In either case, in the preferred embodiment in FIG. (17), apparatusproduces a beam of electromagnetically neutralized wave-particlebehaving entities which is coherently transmitted by coherenttransmission apparatus to a target (block comprising the dashed lineformat), such that adverse electromagnetic interaction of the beam ofelectromagnetically neutralized wave-particle behaving entities withelectromagnetically functional entities comprised in the coherenttransmission apparatus is eliminated to an extent. Wherein, the adverseelectromagnetic effects of transmitting energy for the respectiveapplication are eliminated to an extent. Here, more specifically, thetarget comprises incoherently scattering and transmitting apparatus, anda separate posteriorly located electromagnetic-type utilizing apparatus.

Then, the beam of electromagnetically neutralized wave-particle behavingentities is incoherently scattered to an extent by incoherentlyscattering apparatus so to produce a beam of electromagneticallyfunctional wave-particle behaving entities (which comprises a non-zeromagnitude of time-average electric flux density) in the incoherentlyscattering and transmitting apparatus (i.e., a beam ofelectromagnetically functional wave-particle behaving entities isproduced comprising electromagnetically functional wave-particlebehaving entities produced by incoherent scattering or also comprisingany remaining portion of a beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities which is not incoherently scattered if a beam ofpartly electromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities is applied).

Also, in this step, an extent of such a beam of electromagneticallyfunctional wave-particle behaving entities produced is transmitted bytransmitting apparatus comprised in the target to electromagnetic-typeutilizing apparatus comprising electromagnetically functional entitieswhich utilizes the transmitted beam of electromagnetically functionalwave-particle behaving entities by way of electromagnetic interaction toproduce the result of the respective preferred embodiment.

(Note, if a beam of totally electromagnetically neutralizedwave-particle behaving entities is applied in the preferred embodimentin FIG. (17), then electromagnetic-type incoherent scattering ofelectromagnetically functional wave-particle behaving entities byelectromagnetic-type incoherently scattering apparatus would occurdependent upon the onset of the production of the electromagneticallyfunctional wave-particle behaving entities by potential-energy-typeincoherent scattering. However, if a beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities is applied in the preferred embodiment in FIG. (17),then electromagnetic-type incoherent scattering of electromagneticallyfunctional wave-particle behaving entities by electromagnetic-typeincoherently scattering apparatus would occur independent of the onsetof the production of the electromagnetically functional wave-particlebehaving entities by potential-energy-type incoherent scattering, sincea beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities alreadycomprises wave-particle behaving entities which are partlyelectromagnetically functional.)

FIG. (18) shows another preferred embodiment which is applied for thetransmission and subsequent utilization of energy in an effectivemanner. The preferred embodiment in FIG. (18) applies the steps appliedin the preferred embodiment in FIG. (17) with some modifications. Here,however, the target comprises an incoherently scattering andtransmitting apparatus, specifically comprising, in addition,electromagnetically functional entities; and a separateelectromagnetic-type utilizing apparatus located posteriorly.

In the preferred embodiment in FIG. (18), apparatus produces a beam ofelectromagnetically neutralized wave-particle behaving entities which iscoherently transmitted by coherent transmission apparatus to a target,such that adverse electromagnetic interaction of the beam ofelectromagnetically neutralized wave-particle behaving entities withelectromagnetically functional entities comprised in the coherenttransmission apparatus is eliminated to an extent. Wherein, the adverseelectromagnetic effects of transmitting energy for the respectiveapplication are eliminated to an extent.

Then, the coherently transmitted beam of electromagnetically neutralizedwave-particle behaving entities is incoherently scattered to an extentby respective incoherently scattering apparatus so to produce a beam ofelectromagnetically functional wave-particle behaving entities (whichcomprises a non-zero magnitude of time-average electric flux density)(i.e., a beam of electromagnetically functional wave-particle behavingentities is produced comprising electromagnetically functionalwave-particle behaving entities produced by incoherent scattering oralso comprising any remaining portion of a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities which is not incoherentlyscattered if a beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities isapplied).

Also, in this step, an extent of such a beam of electromagneticallyfunctional wave-particle behaving entities produced is transmitted bytransmission apparatus comprised in the target to electromagneticallyfunctional entities comprised in the apparatus comprising theincoherently scattering and transmitting apparatus, andelectromagnetically functional entities; and also an extent of such abeam of electromagnetically functional wave-particle behaving entitiesis transmitted by transmission apparatus to electromagneticallyfunctional entities comprised in electromagnetic-type utilizingapparatus located posteriorly.

Here, an extent of such a transmitted beam of electromagneticallyfunctional wave-particle behaving entities can be utilized by way ofelectromagnetic interaction by the electromagnetically functionalentities (e.g., electrically charged particles) comprised in theapparatus located anterior to (before) the posteriorly locatedelectromagnetic-type utilizing apparatus to accomplish the objective ofthe respective application of the present invention; or an extent ofsuch a transmitted beam of electromagnetically functional wave-particlebehaving entities produced can be adversely absorbed by way ofelectromagnetic interaction by such electromagnetically functionalentities comprised in the respective anteriorly located apparatus, andthus hinder the accomplishment of the objective of the respectiveapplication of the present invention. Nevertheless, electromagnetic-typeutilizing apparatus located posteriorly then utilizes transmittedelectromagnetically functional wave-particle behaving entities by way ofelectromagnetic interaction to produce the result of the respectivepreferred embodiment (i.e., an extent of the respectively transmittedelectromagnetically functional wave-particle behaving entities producedby incoherent scattering or also an extent of any respectivelytransmitted remaining portion of a beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities which was not incoherently scattered, if a beam ofpartly electromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities is applied, are utilized byway of electromagnetic interaction by electromagnetic-type utilizingapparatus to produce the result of the respective preferred embodiment).

FIG. (19) shows another preferred embodiment which is applied for thetransmission and subsequent utilization of energy in an effectivemanner. The preferred embodiment in FIG. (19) applies the steps appliedin the preferred embodiment in FIG. (17) except that theelectromagnetic-type utilizing apparatus is located at some anterior orlateral location to the incoherently scattering apparatus as the oneshown in an arbitrary lateral location in FIG. (19).

Wherein, in the preferred embodiment in FIG. (19), apparatus produces abeam of electromagnetically neutralized wave-particle behaving entitieswhich is coherently transmitted by coherent transmission apparatus to atarget (comprising incoherently scattering and transmitting apparatus),such that adverse electromagnetic interaction of the beam ofelectromagnetically neutralized wave-particle behaving entities withelectromagnetically functional entities comprised in the coherenttransmission apparatus is eliminated to an extent. Wherein, the adverseelectromagnetic effects of transmitting energy for the respectiveapplication are eliminated to an extent.

Then, the incoherently scattering apparatus comprised in the targetincoherently scatters the coherently transmitted beam ofelectromagnetically neutralized wave-particle behaving entitieslaterally to an extent so to produce a beam of electromagneticallyfunctional wave-particle behaving entities (which comprises a non-zeromagnitude of time-average electric flux density) comprisingelectromagnetically functional wave-particle behaving entities which areproduced by incoherent scattering (or also comprising any laterallydeflected remaining portion of a beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities which is not incoherently scattered if a beam ofpartly electromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities is applied).

Also, in this step, an extent of such a beam of electromagneticallyfunctional wave-particle behaving entities produced is transmitted bytransmission apparatus comprised in the incoherently scattering andtransmitting apparatus (or also comprised in electromagnetic-typeutilizing apparatus) to an electromagnetic-type utilizing apparatuslocated laterally in the target. Wherein, the electromagnetic-typeutilizing apparatus comprising electromagnetically functional entitiesthen utilizes such transmitted electromagnetically functionalwave-particle behaving entities by way of electromagnetic interaction toproduce the result of the respective preferred embodiment.

FIG. (20) shows another preferred embodiment which is applied for thetransmission and subsequent utilization of energy in an effectivemanner. The preferred embodiment in FIG. (20) applies the steps appliedin the preferred embodiment in FIG. (17) except that target apparatuscombines incoherently scattering and transmitting apparatus withelectromagnetic-type utilizing apparatus into one apparatus and thepreferred embodiment herein respectively combines the steps applied bythe respectively combined apparatus.

In the preferred embodiment in FIG. (20), apparatus produces a beam ofelectromagnetically neutralized wave-particle behaving entities which iscoherently transmitted by coherent transmission apparatus to a target(block comprising the dashed line format), such that adverseelectromagnetic interaction of the beam of electromagneticallyneutralized wave-particle behaving entities with electromagneticallyfunctional entities comprised in the coherent transmission apparatus iseliminated to an extent. Wherein, the adverse electromagnetic effects oftransmitting energy for the respective application are eliminated to anextent.

Then, the coherently transmitted beam of electromagnetically neutralizedwave-particle behaving entities is incoherently scattered to an extentby incoherently scattering apparatus comprised in the target so toproduce a beam of electromagnetically functional wave-particle behavingentities (which comprises a non-zero magnitude of time-average electricflux density) (i.e., a beam of electromagnetically functionalwave-particle behaving entities is produced comprisingelectromagnetically functional wave-particle behaving entities producedby electromagnetic-type and potential-energy-type incoherent scatteringor also comprising any remaining portion of a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities which is not incoherentlyscattered if a beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities isapplied). Also, in this step, transmission apparatus in the targettransmits an extent of such a beam of electromagnetically functionalwave-particle behaving entities to electromagnetic-type utilizingapparatus located in, or posterior to, the array of incoherentlyscattering and transmitting particle beams. Subsequently, theelectromagnetic-type utilizing apparatus, comprising electromagneticallyfunctional entities, utilizes transmitted electromagnetically functionalwave-particle behaving entities by way of electromagnetic interaction toproduce the result of the preferred embodiment.

FIG. (21) shows another preferred embodiment which is applied for thetransmission and subsequent utilization of energy in an effectivemanner. Steps comprised in the preferred embodiment in FIG. (17) can beapplied in the preferred embodiment in FIG. (21) with somemodifications.

Wherein, in the preferred embodiment in FIG. (21), apparatus produces abeam of electromagnetically neutralized wave-particle behaving entities(which is pulsed or continuous) which comprises electromagneticallyneutralized wave-particle behaving entities which individually andcollectively comprise potential energy so to effectively produce anincoherently scattering and transmitting apparatus (e.g., a beam ofelectromagnetically neutralized wave-particle behaving electrons). Then,the beam of electromagnetically neutralized wave-particle behavingentities is coherently transmitted by coherent transmission apparatus toa focus positioned anterior to, or inside of, an electromagnetic-typeutilizing apparatus in a target (block comprising the dashed lineformat), such that adverse electromagnetic interaction of the beam ofelectromagnetically neutralized wave-particle behaving entities withelectromagnetically functional entities comprised in the coherenttransmission apparatus is eliminated to an extent. Wherein, the adverseelectromagnetic effects of transmitting energy for the respectiveapplication are eliminated to an extent.

Subsequently, the beam of electromagnetically neutralized wave-particlebehaving entities is incoherently scattered to an extent by incoherentlyscattering apparatus so to produce a beam of electromagneticallyfunctional wave-particle behaving entities (which comprises a non-zeromagnitude of time-average electric flux density) in theelectromagnetic-type utilizing apparatus. Here, incoherently scatteringapparatus comprises potential-energy-type incoherently scatteringapparatus comprising wave-particle behaving entities which comprise acollective potential energy at the focus of the beam ofelectromagnetically neutralized wave-particle behaving entities (whichhas potential-energy-type incoherent scattering parameters equivalent tothose pertinent to the preferred embodiment in FIG. (13)); or alsoincoherently scattering apparatus comprising electromagnetic-type (e.g.,electrostatic-type) incoherently scattering apparatus comprised in, forexample, a beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving electricallycharged particles (which would comprise a non-zero magnitude oftime-average electric flux density) at the focus anterior to, or insideof, the electromagnetic-type utilizing apparatus (if a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving electrically charged particles isapplied) (which has electromagnetic-type incoherent scatteringparameters equivalent to those pertinent to the preferred embodiment inFIG. (14)). Also, in this step, an extent of such a beam ofelectromagnetically functional wave-particle behaving entities producedis transmitted by transmission apparatus comprised in the beam ofelectromagnetically neutralized wave-particle behaving entities or alsocomprised in the electromagnetic-type utilizing apparatus. Then, theelectromagnetic-type utilizing apparatus comprising electromagneticallyfunctional entities utilizes transmitted electromagnetically functionalwave-particle behaving entities by way of electromagnetic interaction toproduce the result of the respective preferred embodiment.

FIG. (22) shows another preferred embodiment which is applied for thetransmission and subsequent utilization of energy in an effectivemanner. Here, this preferred embodiment applies the steps applied in thepreferred embodiment in FIG. (17) except that, differently, thepreferred embodiment herein comprises an incoherently scattering andtransmitting apparatus which comprises another particle beam (i.e., anincoherent scattering and transmitting beam of wave-particle behavingentities which is collimated or focused and continuous or pulsed).

In the preferred embodiment in FIG. (22), apparatus produces a beam ofelectromagnetically neutralized wave-particle behaving entities which iscoherently transmitted by coherent transmission apparatus to a target inwhich the other particle beam (i.e., the incoherently scattering andtransmitting apparatus) is propagating, such that adverseelectromagnetic interaction of the beam of electromagneticallyneutralized wave-particle behaving entities with electromagneticallyfunctional entities comprised in the coherent transmission apparatus iseliminated to an extent. Wherein the adverse electromagnetic effects oftransmitting energy are eliminated to an extent.

Then, the coherently transmitted beam of electromagnetically neutralizedwave-particle behaving entities is incoherently scattered to an extentby incoherently scattering apparatus so to produce a beam ofelectromagnetically functional wave-particle behaving entities (whichcomprises a non-zero magnitude of time-average electric flux density) inthe target (i.e., a beam of electromagnetically functional wave-particlebehaving entities is produced comprising electromagnetically functionalwave-particle behaving entities produced by incoherent scattering oralso comprising any remaining portion of a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities which is not incoherentlyscattered if a beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities isapplied). Here, the incoherently scattering apparatus, comprisinganother particle beam comprises: potential-energy-type incoherentlyscattering and transmitting apparatus or also electromagnetic-typeincoherently scattering and transmitting apparatus if a beam oftransmission energy comprising a beam of totally electromagneticallyneutralized wave-particle behaving entities is applied; orpotential-energy-type incoherently scattering and transmitting apparatusand/or electromagnetic-type incoherently scattering and transmittingapparatus if a beam of transmission energy comprising a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities is applied. Wherein,potential-energy-type incoherently scattering apparatus comprises anyparticle beam which comprises wave-particle behaving entities whichindividually and collectively comprise potential energy, andelectromagnetic-type incoherent scattering apparatus comprises anyparticle beam which comprises wave-particle behaving entities whichcomprise waves which constructively interfere to an extent withassociated electric and magnetic fields which respectively reinforce toan extent (i.e., a beam of totally electromagnetically functionalwave-particle behaving entities or a beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities). Wherein, such incoherently scattering andtransmitting apparatus would comprise incoherent scattering parametersequivalent to those described in the preferred embodiment in FIG. (13)or also (14) or (13) and/or (14) depending upon the type of beam ofelectromagnetically neutralized wave-particle behaving entities appliedand the type of incoherently scattering and transmitting media applied.

Also, in this step, transmission apparatus comprised by the otherparticle beam (i.e., the incoherently scattering and transmittingapparatus) (or also comprised in the electromagnetic-type utilizingapparatus) transmits an extent of such a beam of electromagneticallyfunctional wave-particle behaving entities produced toelectromagnetic-type utilizing apparatus. Subsequently, theelectromagnetic-type utilizing apparatus which compriseselectromagnetically functional entities and is located in, or posteriorto, the path of the incoherent scattering and transmitting beam,utilizes transmitted electromagnetically functional wave-particlebehaving entities by way of electromagnetic interaction to produce theresult of the respective preferred embodiment

Other preferred embodiments can include a plural number (an array) ofother particle beams (e.g., a targeted array of intersecting particlebeams such as a grid of particle beams) which are each collimated orfocused and continuous or pulsed, or a combination of such particlebeams as incoherent scattering (and transmitting) apparatus. Wherein,each particle beam comprised by such a plurality of particle beamscomprises the parameters comprised by the incoherent scattering andtransmitting beam applied in the preferred embodiment in FIG. (22).

Wherein, in such a preferred embodiment, apparatus produces a beam ofelectromagnetically neutralized wave-particle behaving entities which iscoherently transmitted by coherent transmission apparatus to a target inwhich a plurality of such particle beams (comprising incoherentscattering or also transmitting apparatus) are propagating, such thatadverse electromagnetic interaction of the beam of electromagneticallyneutralized wave-particle behaving entities with electromagneticallyfunctional entities comprised in the coherent transmission apparatus iseliminated to an extent. Wherein, the adverse electromagnetic effects oftransmitting energy are eliminated to an extent.

Subsequently, the coherently transmitted beam of electromagneticallyneutralized wave-particle behaving entities is incoherently scattered toan extent by incoherently scattering apparatus (i.e., the plurality ofother particle beams) so to produce a beam of electromagneticallyfunctional wave-particle behaving entities (comprising a non-zeromagnitude of time-average electric flux density) (i.e., a beam ofelectromagnetically functional wave-particle behaving entities isproduced comprising electromagnetically functional wave-particlebehaving entities produced by incoherent scattering or also comprisingany remaining portion of a beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities which is not incoherently scattered if a beam ofpartly electromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities is applied).

Also, in this step, transmitting apparatus comprised in the respectiveparticle beam array (or also comprised in the electromagnetic-typeutilizing apparatus transmits an extent of such a beam ofelectromagnetically functional wave-particle behaving entities toelectromagnetic-type utilizing apparatus. Finally, electromagnetic-typeutilizing apparatus comprising electromagnetically functional entitiesutilizes transmitted electromagnetically functional wave-particlebehaving entities by way of electromagnetic interaction to produce theresult of the respective preferred embodiment.

FIG. (23) is another preferred embodiment for the transmission of energyin an effective manner. Steps 1) and 2) comprised in the preferredembodiment in FIG. (2) or (6) can be applied in the preferred embodimentin FIG. (23) except the coherent transmission apparatus (dashed line inthe shape of a block) in the preferred embodiment in FIG. (23), inaddition, comprises a filtering apparatus. Wherein, in the preferredembodiment in FIG. (23), apparatus produces a beam ofelectromagnetically neutralized wave-particle behaving entities which iscoherently transmitted by coherent transmitting apparatus comprised in afiltering apparatus to a target, such that adverse electromagneticinteraction of the beam of electromagnetically neutralized wave-particlebehaving entities with electromagnetically functional entities comprisedin the coherent transmission apparatus is eliminated to an extent.Wherein, the adverse electromagnetic effects of transmitting energy areeliminated to an extent.

Wherein, the filtering apparatus coherently transmits the respectivebeam of electromagnetically neutralized wave-particle behaving entitiesand eliminates unwanted electromagnetically functional wave-particlebehaving entities from the beam of electromagnetically neutralizedwave-particle behaving entities which may be produced by systematicand/or random error (e.g., for protection in health care applications ofthe present invention). Here, a filtering apparatus can comprise:

a) a passive-type filtering apparatus which comprises coherentlytransmissive electromagnetically absorptive apparatus for an embodimentof the present invention which uses a beam of totallyelectromagnetically neutralized electromagnetic field quanta, such thatsuch a filtering apparatus would coherently transmit the beam of totallyelectromagnetically neutralized electromagnetic field quanta applied andelectromagnetically absorb unwanted electromagnetically functionalelectromagnetic field quanta (produced by systematic and/or randomerror) from the respective beam of totally electromagneticallyneutralized electromagnetic field quanta applied (e.g., a filteringapparatus can include coherently transmissive resonance absorptiveapparatus for absorbing relatively long wavelength electromagnetic fieldquanta or coherently transmissive edge absorptive apparatus forabsorbing relatively short wavelength electromagnetic field quanta,e.g., X-rays) from a respectively applied beam of (totally)electromagnetically neutralized wave-particle behaving entities;

b) a passive-type filtering apparatus which comprises coherentlytransmissive apparatus which comprises electrostatically,electromagnetically, or magnetically deflecting apparatus in combinationwith electromagnetically absorptive apparatus, such that such afiltering apparatus would deflect unwanted electromagneticallyfunctional electrically charged wave-particle behaving entities(produced by systematic and/or random error) out of a respective beam of(totally) electromagnetically neutralized wave-particle behavingelectrically charged particles applied towards the electromagneticallyabsorptive apparatus which would subsequently absorb the deflectedunwanted electromagnetically functional electrically charged particlesby way of electromagnetic interaction or incoherently scatter, transmit,and then absorb by way of electromagnetic interaction unwantedelectromagnetically functional electrically charged particles if partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving electrically charged particles aredeflected out a beam of (totally) electromagnetically neutralizedwave-particle behaving electrically charged particles; or

c) an active-type filtering apparatus which comprises a coherentlytransmissive limiter-type apparatus for an embodiment of the presentinvention which applies a beam of partly electromagnetically neutralizedand partly electromagnetically functional wave-particle behavingentities (e.g., an optical limiter for an embodiment which applies abeam of partly electromagnetically neutralized and partlyelectromagnetically functional electromagnetic field quanta). Wherein, abeam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities appliedin a given embodiment would be coherently transmitted, and its electricflux density (intensity) respectively limited by the limiter-typefiltering apparatus, such that unwanted electromagnetically functionalwave-particle behaving entities (produced by systematic and/or randomerror) would be eliminated from the respectively applied beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities applied.

FIG. (24) shows an embodiment of the present invention as described inthe preferred embodiment in FIG. (1) surrounded by shielding apparatus.When circumstances warrant, proper safety measures should be implementedsuch as using shielding to prevent unwanted irradiating of any givenmaterial or space.

The shielding apparatus (drawn generally in the form of a block) canenclose the entire embodiment of the present invention as shown in FIG.(24), or the shielding apparatus can be used between only part of agiven embodiment of the present invention and any given material orspace. Such shielding can include: a) incoherently scattering apparatuscomprising potential-energy-type incoherently scattering apparatus andelectromagnetic-type incoherently scattering apparatus in combinationwith an electromagnetically absorptive apparatus; or b) a potentialenergy barrier under the appropriate circumstances (e.g., when a givenpotential energy barrier applied can withstand the electromagneticeffects which may result from the impinging beam to be shielded from(e.g., nuclear fusion or material dissociation). Wherein, here, anyelectromagnetically neutralized wave-particle behaving entity (orentities) or electromagnetically functional wave-particle behavingentity (or entities) which transgresses (or which transgress) beyond adesired boundary in the surroundings of an embodiment of the presentinvention would be absorbed by shielding apparatus (i.e., for anelectromagnetically functional wave-particle behaving entity, orentities) or incoherently scattered such that electromagneticallyfunctional electromagnetic field quanta, comprising a non-zerotime-average electric flux density, are produced and transmitted bytransmitting media to, and then absorbed by way of electromagneticinteraction by, electromagnetically absorptive apparatus comprisingelectrically charged particles comprised by shielding apparatus (i.e.,for electromagnetically neutralized wave-particle behaving entities).(Note, under respectively appropriate circumstances, shielding apparatuscan comprise, as examples: a) a stationary-type of shielding apparatuscomprising particles with respective parameters as applied in preferredembodiments comprised in FIGS. (39) and (45); or b) under certaincircumstances shielding apparatus can comprise a plural number, i.e., anarray, of particle beams, e.g., a targeted array of intersectingparticle beams such as a grid of particle beams, which are eachcollimated or focused and continuous or pulsed, or a combination of suchparticle beams which comprise incoherent scattering, but nottransmitting, apparatus.)

There are different ways of adjusting the present invention toaccomplish the result of the respective application of the presentinvention including particle flux density adjustment; electric fluxdensity adjustment; focal point adjustment; and other forms of adjustingthe present invention. One or more of such ways of adjusting the presentinvention can be applied to accomplish the desired result of therespective application of the present invention depending on theconditions of the application used.

FIGS. (25A) and (25B) show two embodiments of the present inventionwhich together represent the significance of adjusting the particle fluxdensity of a beam of totally electromagnetically neutralizedwave-particle behaving entities. In each of the two embodiments in FIGS.(25A) and (25B), apparatus produces a beam of totallyelectromagnetically neutralized wave-particle behaving entities. Thebeams of totally electromagnetically neutralized wave-particle behavingentities in the two embodiments are equivalent (comprising equivalentwave-particle behaving entities with equivalent wavelengths) except thatthe magnitude of time-average particle flux density in each beam oftotally electromagnetically neutralized wave-particle behaving entitiesis different.

The beams of totally electromagnetically neutralized wave-particlebehaving entities in FIGS. (25A) and (25B) are coherently transmitted byequivalent coherent transmission apparatus to incoherently scatteringand transmitting apparatus. The incoherently scattering and transmittingapparatus in both the embodiments comprise equivalent apparatus(comprising a uniform distribution of potential-energy-type incoherentlyscattering and transmitting apparatus, and electromagnetic-typeincoherently scattering and transmitting apparatus) which eachcompletely scatters the beam of totally electromagnetically neutralizedwave-particle behaving entities applied in a respective embodiment in anincoherent manner.

In each of the embodiments, a beam of electromagnetically functionalwave-particle behaving entities (which comprises a non-zero magnitude oftime-average electric flux density) is produced by complete incoherentscattering, is transmitted up to and through the center of the exitplane of the respective incoherently scattering and transmittingapparatus, and is represented arbitrarily by its own standard normaldistribution curve. Both standard normal distribution curves are plottedin a respective (x-y) plane along a respective (y) axis, which isaligned with the center of the exit plane of the respective incoherentlyscattering and transmitting apparatus, and each curve is separatelyplotted along a respective (x) axis. In each embodiment in FIGS. (25A)and (25B), a line is tangent to the maximum time-average electric fluxdensity on the respective standard normal distribution curve andintersects the respective (x) axis at a point.

Since the time-average particle flux density in the beam of totallyelectromagnetically neutralized wave-particle behaving entities in FIG.(25A) is less than the time-average particle flux density in the beam oftotally electromagnetically neutralized wave-particle behaving entitiesin FIG. (25B), the maximum time-average electric flux density producedin incoherently scattering and transmitting apparatus in the firstembodiment in FIG. (25A) along the respective exit plane is less thanthe maximum time-average electric flux density produced in incoherentlyscattering and transmitting apparatus along the respective exit plane inFIG. (25B). Thus, the distance on the (x) axis between (0) (zero) andthe intersecting point of the line tangent to the time-average electricflux density standard normal distribution curve in FIG. (25A) is lessthan the distance on the (x) axis between (0) (zero) and theintersecting point of the line tangent to the time-average electric fluxdensity standard normal distribution curve in FIG. (25B). Here, forexample, time-average particle flux density adjustment is accomplishedby changing the power setting of the source or sources of the given beamof electromagnetically neutralized wave-particle behaving entities.(Note, refer to the note in the preferred embodiment in FIG. (1) for thedetermination of time-average particle flux density.)

FIGS. (26A) and (26B) show two embodiments of the present inventionwhich together represent the significance of adjusting the particle fluxdensity of a beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities. In eachof the two embodiments in FIGS. (26A) and (26B), apparatus produces abeam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities. Thebeams of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities in thetwo embodiments each comprise equivalent wave-particle behaving entitieswith equivalent wavelengths; each comprise a different magnitude oftime-average particle flux density; each comprise a different magnitudeof time-average electric flux density, and, yet, each comprises wavecomponents which comprise the same relative phase relation.

The beams of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities in FIGS.(26A) and (26B) are coherently transmitted by equivalent coherenttransmission apparatus to incoherently scattering and transmittingapparatus. The incoherently scattering and transmitting apparatus inboth the embodiments comprise equivalent apparatus (comprising a uniformdistribution of potential-energy-type incoherently scattering andtransmitting apparatus, and electromagnetic-type incoherently scatteringand transmitting apparatus) which each completely scatters the beam ofpartly electromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities applied in the respectiveembodiments in an incoherent manner.

In each of the embodiments, a beam of electromagnetically functionalwave-particle behaving entities (which comprises a non-zero magnitude oftime-average electric flux density) is produced by complete incoherentscattering, is transmitted up to and through the center of the exitplane of a respective incoherently scattering and transmittingapparatus, and is represented arbitrarily by its own standard normaldistribution curve. Both standard normal distribution curves are plottedin a respective (x-y) plane along a respective (y) axis, which isaligned with the center of the exit plane of the respective incoherentlyscattering and transmitting apparatus, and each curve is separatelyplotted along a respective (x) axis. In each embodiment in FIGS. (26A)and (26B), a line is tangent to the maximum time-average electric fluxdensity on the respective standard normal distribution curve andintersects the respective (x) axis at a point.

Since the time-average particle flux density in the beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities in FIG. (26A) is less thanthe time-average particle flux density in the beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities in FIG. (26B), the maximumtime-average electric flux density produced in incoherently scatteringand transmitting apparatus in the embodiment in FIG. (26A) along therespective exit plane is less than the maximum time-average electricflux density produced in incoherently scattering and transmittingapparatus along the respective exit plane in the embodiment in FIG.(26B). Thus, the distance on the (x) axis between (0) (zero) and theintersecting point of the line tangent to the time-average electric fluxdensity standard normal distribution curve in the embodiment in FIG.(26A) is less than the distance on the (x) axis between (0) (zero) andthe intersecting point of the line tangent to the time-average electricflux density standard normal distribution curve in the embodiment inFIG. (26B). Here, for example, the time-average particle flux densityadjustment is accomplished by changing the power setting of the sourceor sources of the given beam of electromagnetically neutralizedwave-particle behaving entities. (Note, that the time-average electricflux density of a beam of partly electromagnetically neutralized andpartly electromagnetically functional wave-particle behaving entitiescan be adjusted by changing the amplitude of the wave components whichit consists of by, for example, changing the power setting of the sourceor sources which produces such beam components. Also, refer to the notein the preferred embodiment in FIG. (1) for the determination oftime-average particle flux density.)

FIGS. (27A) and (27B) show two embodiments of the present inventionwhich together represent one aspect of the significance of adjusting thetime-average electric flux density of the present invention. In theembodiment in FIG. (27A), apparatus produces a beam of totallyelectromagnetically neutralized wave-particle behaving entities, and inthe embodiment in FIG. (27B), apparatus produces a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities.

The beams of electromagnetically neutralized wave-particle behavingentities in the two embodiments in FIGS. (27A) and (27B) each compriseequivalent wave-particle behaving entities with equivalent wavelength;each comprise an equal magnitude of time-average particle flux density;and each comprise a different magnitude of time-average electric fluxdensity; and each comprise wave components which comprise a differentrelative phase relation.

The beams of electromagnetically neutralized wave-particle behavingentities in each of the two embodiments in FIGS. (27A) and (27B) arecoherently transmitted by equivalent coherent transmission apparatus toincoherently scattering and transmitting apparatus. The incoherentlyscattering and transmitting apparatus in both the embodiments compriseequivalent apparatus (comprising a uniform distribution ofpotential-energy-type incoherently scattering and transmittingapparatus, and electromagnetic-type incoherently scattering andtransmitting apparatus) which each completely scatters the beam ofelectromagnetically neutralized wave-particle behaving entities appliedin the respective embodiment in an incoherent manner.

In each of the embodiments, a beam of electromagnetically functionalwave-particle behaving entities) which comprises a non-zero magnitude oftime-average electric flux density) is produced by complete incoherentscattering, is transmitted up to and through the center of the exitplane of a respective incoherently scattering and transmittingapparatus, and is represented arbitrarily by its own standard normaldistribution curve. Both standard normal distribution curves are plottedin a respective (x-y) plane along a respective (y) axis, which isaligned with the center of the exit plane of the respective incoherentlyscattering and transmitting apparatus, and each curve is separatelyplotted along a respective (x) axis. In each embodiment, a line istangent to the maximum time-average electric flux density on therespective standard normal distribution curve and intersects therespective (x) axis at a point.

Since the time-average particle flux density in the beam of totallyelectromagnetically neutralized wave-particle behaving entities in theembodiment in FIG. (27A) is equal to the time-average particle fluxdensity in the beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities in theembodiment in FIG. (27B), the maximum time-average electric flux densityproduced in incoherently scattering and transmitting apparatus in theembodiment in FIG. (27A) along the respective exit plane is equal to themaximum time-average electric flux density produced in incoherentlyscattering and transmitting apparatus along the respective exit plane inthe embodiment in FIG. (27B) (neglecting the effects of anyattenuation). Thus, the distance on the (x) axis between (0) (zero) andthe intersecting point of the line tangent to the time-average electricflux density standard normal distribution curve in the embodiment inFIG. (27A) is equal to the distance on the (x) axis between (0) (zero)and the intersecting point of the line tangent to the time-averageelectric flux density standard normal distribution curve in theembodiment in FIG. (27B).

The equality of the maximum time-average electric flux densities existsirrespective of the difference in the time-average electric fluxdensities of the respective beams produced by phase adjustment, sincethe incoherently scattering apparatus in each embodiment in FIGS. (27A)and (27B) completely incoherently scatters the beam ofelectromagnetically neutralized wave-particle behaving entities appliedin the respective embodiment. (Note, time-average electric flux densityadjustment is accomplished by changing the relative phase of the waves(i.e., herein, by changing the relative phase relation of the wavecomponents) which are in a respectively applied beam ofelectromagnetically neutralized wave-particle behaving entities.)

FIGS. (28A) and (28B) show two embodiments of the present inventionwhich together represent another aspect of the significance of adjustingthe time-average electric flux density of the present invention. In theembodiment in FIG. (28A), apparatus produces a beam of totallyelectromagnetically neutralized wave-particle behaving entities, and inthe embodiment in FIG. (28B), apparatus produces a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities. The beams ofelectromagnetically neutralized wave-particle behaving entities in thetwo embodiments in FIGS. (28A) and (28B) each comprises equivalentwave-particle behaving entities with equivalent wavelengths; eachcomprises an equal magnitude of time-average particle flux density; eachcomprises a different magnitude of time-average electric flux density;and each comprises wave components which comprise a different relativephase relation.

The beams of electromagnetically neutralized wave-particle behavingentities in each of the two embodiments in FIGS. (28A) and (28B) arecoherently transmitted by equivalent coherent transmission apparatus toincoherently scattering and transmitting apparatus. The incoherentlyscattering and transmitting apparatus in both the embodiments compriseequivalent apparatus (comprising a uniform distribution ofpotential-energy-type incoherently scattering and transmittingapparatus, and electromagnetic-type incoherently scattering andtransmitting apparatus). However, in this aspect of time-averageelectric flux adjustment, each incoherently scattering apparatus onlypartly scatters the respective beam of electromagnetically neutralizedwave-particle behaving entities applied in the respective embodiment inan incoherent manner.

In each of the embodiments, a beam of electromagnetically functionalwave-particle behaving entities (which comprises a non-zero magnitude oftime-average electric flux density) is produced by partial incoherentscattering, is transmitted up to and through the center of the exitplane of a respective incoherently scattering and transmittingapparatus, and is represented arbitrarily by its own standard normaldistribution curve. Both standard normal distribution curves are plottedin a respective (x-y) plane along a respective (y) axis, which isaligned with the center of the exit plane of the respective incoherentlyscattering and transmitting apparatus, and each curve is separatelyplotted along a respective (x) axis. In each embodiment in FIGS. (28A)and (28B), a line is tangent to the maximum time-average electric fluxdensity on the respective standard normal distribution curve andintersects the respective (x) axis at a point.

Here, even though the time-average particle flux density in the beam oftotally electromagnetically neutralized wave-particle behaving entitiesin the embodiment in FIG. (28A) is equal to the time-average particleflux density in the beam of partly electromagnetically neutralized andpartly electromagnetically functional wave-particle behaving entities inthe embodiment in FIG. (28B), the incoherently scattering apparatus ineach embodiment only partly incoherently scatters the respective beam ofelectromagnetically neutralized wave-particle behaving entities appliedin the respective embodiment, and thus the incoherent scattering ofelectromagnetically functional wave-particle behaving entities byelectromagnetic-type incoherently scattering apparatus has a greatereffect in the embodiment in FIG. (28B) which applies the beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities, since the beam of partlyelectromagnetically functional wave-particle behaving entities comprisespartly electromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities which facilitates theelectromagnetic-type incoherent scattering in the electromagnetic-typeincoherently scattering apparatus.

Thus, the maximum time-average electric flux density produced in theincoherently scattering and transmitting apparatus in the embodiment inFIG. (28A) along the respective exit plane is less than the maximumtime-average electric flux density produced in incoherently scatteringand transmitting apparatus in the embodiment in FIG. (28B) along therespective exit plane. Thus, the distance between (0) (zero) and theintersecting point of the line tangent to the time-average electric fluxdensity standard normal distribution curve in the embodiment in FIG.(28A) is less than the distance between (0) (zero) and the intersectingpoint of the line tangent to the time-average electric flux densitystandard normal distribution curve in the embodiment in FIG. (28B).(Note that here, also, time-average electric flux density adjustment isaccomplished by changing the relative phase of the waves (i.e., herein,by changing the relative phase relation of the wave components) whichare in a respectively applied beam of electromagnetically neutralizedwave-particle behaving entities.)

FIGS. (29A) and (29B) show two embodiments of the present inventionwhich together represent the significance of adjusting the position ofthe focal point of the present invention. In the two embodiments inFIGS. (29A) and (29B), apparatus produce equivalent beams ofelectromagnetically neutralized wave-particle behaving entities whicheach comprise equivalent wave-particle behaving entities with equivalentwavelength; each comprise an equal magnitude of time-average particleflux density; and each comprise an equal magnitude of time-averageelectric flux density.

The beams of electromagnetically neutralized wave-particle behavingentities in each of the two embodiments in FIGS. (29A) and (29B) arecoherently transmitted by equivalent coherent transmission apparatus toa respective focus in equivalent incoherently scattering andtransmitting apparatus (comprising a uniform distribution ofpotential-energy-type incoherently scattering and transmittingapparatus, and electromagnetic-type incoherently scattering andtransmitting apparatus). In each of the embodiments, a beam ofelectromagnetically functional wave-particle behaving entities (whichcomprises a non-zero magnitude of time-average electric flux density) isproduced to a respective extent by incoherent scattering, is transmittedup to and through the center of the focal plane in the respectiveincoherently scattering and transmitting apparatus, and is representedarbitrarily by its own standard normal distribution curve. Both standardnormal distribution curves are plotted in a respective (x-y) plane alonga respective (y) axis, which is aligned with the focal plane in therespective incoherently scattering and transmitting apparatus, and eachcurve is separately plotted along a respective (x) axis. In eachembodiment in FIGS. (29A) and (29B), a line is tangent to the maximumtime-average electric flux density on the respective standard normaldistribution curve and intersects the respective (x) axis at a point.

Here, the focal point of the beam of electromagnetically neutralizedwave-particle behaving entities in the embodiment in FIG. (29A) ispositioned at a lesser depth into the respective incoherently scatteringand transmitting apparatus than the depth of the focal point of the beamof electromagnetically neutralized wave-particle behaving entities ispositioned into the respective incoherently scattering and transmittingapparatus in the embodiment in FIG. (29B). Thus, the number ofincoherent scattering sources in the path of the beam ofelectromagnetically neutralized wave-particle behaving entities anteriorto the focus in the embodiment in FIG. (29A) is less than the number ofincoherent scattering sources in the path of the beam ofelectromagnetically neutralized wave-particle behaving entities anteriorto the focus in the embodiment in FIG. (29B).

Thus, the incoherently scattering apparatus in the embodiment in FIG.(29A) incoherently scatters the respectively applied beam ofelectromagnetically neutralized wave-particle behaving entities lessanterior to the focal point than the incoherently scattering apparatusincoherently scatters the respectively applied beam ofelectromagnetically neutralized wave-particle behaving entities anteriorto the focal point in the embodiment in FIG. (29B). Thus, the maximumtime-average electric flux density produced in the incoherentlyscattering and transmitting apparatus along the respective focal planein the embodiment in FIG. (29A) is less than the maximum time-averageelectric flux density produced in the incoherently scattering andtransmitting apparatus along the respective focal plane in theembodiment in FIG. (29B). Thus, the distance between (0) (zero) and theintersecting point of the line tangent to the time-average electric fluxdensity standard normal distribution curve in the embodiment in FIG.(29A) is less than the distance between (0) (zero) and the intersectingpoint of the line tangent to the time-average electric flux densitystandard normal distribution curve in the embodiment in FIG. (29B).

Other ways of adjusting an embodiment of the present invention in orderto accomplish the objective of a respective application include:

a) changing the beam (or beams) of electromagnetically neutralizedwave-particle behaving entities applied such as by changing the typeand/or wavelength of the wave-particle behaving entities applied and/orchanging the shape of the beam applied including whether a beam iscollimated or focused and continuous or pulsed);

b) changing (when practical) the values of the respective parameters ofthe coherent transmission media and/or target media applied in anembodiment including changing the size, spacing, number, and/ordistribution of the respective potential-energy-type incoherentlyscattering apparatus and/or changing the size, spacing, number,distribution and/or resonant frequency (or frequencies) of therespective electromagnetic-type incoherently scattering apparatus;

c) changing the alignment of any beam applied including changing theposition of the beam axis of a beam electromagnetically neutralizedwave-particle behaving entities applied when the target comprises anon-uniform distribution of incoherently scattering apparatus in orderto change the number of the incoherent scattering sources in the path ofthe respective beam of electromagnetically neutralized wave-particlebehaving entities applied, and thus change the number ofelectromagnetically functional wave-particle behaving entities producedby incoherent scattering, and consequentially utilized byelectromagnetic-type utilizing apparatus in a respective target; and/or,

d) changing the diameter of a focused beam of electromagneticallyneutralized wave-particle behaving entities applied when the respectivetarget comprises a significantly dense incoherently scattering apparatusin order to change the number of the incoherent scattering sources inthe path of a respective beam of electromagnetically neutralizedwave-particle behaving entities applied anterior to the focus so tochange the number of electromagnetically functional wave-particlebehaving entities produced by incoherent scattering, and consequentiallyutilized by electromagnetic-type utilizing apparatus in a respectivetarget; or,

e) changing the diameter of any beam of electromagnetically neutralizedwave-particle behaving entities applied when the respective targetcomprises a non-uniform distribution of incoherently scatteringapparatus in order to change the density of the incoherent scatteringsources in the path of a respective beam of electromagneticallyneutralized wave-particle behaving entities applied anterior to theelectromagnetic-type utilizing apparatus so to change the number ofelectromagnetically functional wave-particle behaving entities producedby incoherent scattering, and consequentially utilized byelectromagnetic-type utilizing apparatus in a respective target.

FIG. (30) shows a plan side view of a generalized preferred embodimentof the present invention which is applied for efficient cold nuclearfusion. In this case, the embodiment in FIG. (30) eliminates adverseelectrostatic interaction of nuclear fusion reactants so to eliminatethe adverse electrostatic effect of a lack of nuclear fusion whenattempting to produce nuclear fusion.

The embodiment in FIG. (30), in general, applies the steps applied inthe preferred embodiment in FIG. (2).

The embodiment in FIG. (30) produces cold nuclear fusion as follows:

Step 1) apparatus (2F) (comprising interferometric apparatus comprisinga particle accelerator) produces a beam of totally electromagneticallyneutralized wave-particle behaving nuclear fusion reactants (4F)comprising totally electromagnetically neutralized wave-particlebehaving atomic nuclei (e.g., a beam of totally electromagneticallyneutralized wave-particle behaving protons). The beam of totallyelectromagnetically neutralized wave-particle behaving nuclear fusionreactants (4F) comprises waves which produce total destructiveinterference and time-varying electric and magnetic fields which totallycancel respectively;

Step 2) nuclear fusion reactants from the beam of totallyelectromagnetically neutralized wave-particle behaving nuclear fusionreactants (4F) are coherently transmitted by coherent transmission media(6F) comprising the electrostatic field (or fields) comprised by arespectively targeted nuclear fusion reactant (or respectively targetednuclear fusion reactants) comprised in target (8F) to (or to within asignificant distance of) the respectively target nuclear fusion reactant(or reactants) in target (8F). Wherein, during coherent transmission,the beam of totally electromagnetically neutralized wave-particlebehaving nuclear fusion reactants (4F) comprises waves which producetotal destructive interference with associated time-varying electric andmagnetic fields which totally cancel respectively, such that adverseelectrostatic interaction of nuclear fusion reactants in the beam oftotally electromagnetically neutralized wave-particle behaving nuclearfusion reactants (4F) with the respectively targeted nuclear fusionreactant (or reactants) in target (8F) is significantly eliminated, andthus adverse electrostatic repulsion between nuclear fusion reactants issignificantly eliminated; and,

Step 3) respective nuclear fusion reactants fuse in significantproportions to produce a significant amount of nuclear fusion products.

FIG. (31) shows a plan side view of a generalized preferred embodimentof the present invention which is applied for radiological treatment(e.g., radiosurgery or radiotherapy) in an effective manner. In thiscase, the embodiment in FIG. (31) eliminates an extent of the adverseelectromagnetic interaction of wave-particle behaving entities with softhealthy biological tissue (including any soft healthy amorphousbiological substance) comprised in biological tissue surrounding thetarget of radiological treatment. Hence, an extent of the adverseelectromagnetic effects of transmitting energy for radiologicaltreatment can be eliminated (e.g., an extent of the destruction of softhealthy biological tissue in radiological treatment is eliminated bydecreasing the radiation absorbed dose (RAD) of the respective softhealthy biological tissue, and thus the occurrence of adverse sideeffects of radiological treatment (e.g., cancer) can be decreased to anextent).

Steps pertinent to the preferred embodiment in FIG. (20) are, ingeneral, applied in the preferred embodiment in FIG. (31) with somemodifications. The preferred embodiment in FIG. (31) is applied, morespecifically, according to the following steps:

Step 1) apparatus (2G) (which is isolated from mechanical vibrations)produces a beam of electromagnetically neutralized wave-particlebehaving entities (4G) which comprises, for example, a beam ofelectromagnetically neutralized high energy electrons or a beam ofelectromagnetically neutralized high energy electromagnetic field quanta(e.g., a beam of electromagnetically neutralized X-rays) (which iscontinuous or pulsed and collimated or focused as the pertinentradiological treatment application requires). (Note, one should be awareof the use of a beam of totally electromagnetically neutralizedwave-particle behaving atomic nuclei, e.g., a beam of totallyelectromagnetically neutralized wave-particle behaving protons for coldnuclear fusion in the preferred embodiment in FIG. (30) before choosinga beam of electromagnetically neutralized wave-particle behavingentities to be applied for radiation treatment);

Step 2) the beam of electromagnetically neutralized wave-particlebehaving entities (4G) is coherently transmitted by coherenttransmission media comprising a filter (34G), air (36G), and softhealthy biological tissue (38G) (including any soft healthy amorphousbiological substance) to the target of radiological treatment comprisinga relatively hard treatment site (8G) (rectangular block comprising thedashed line format). Here, the hard treatment site (8G) (e.g., acalcified tumor or pathological bone) is surrounded by biological tissueincluding the soft healthy biological tissue (38G).

In this case, coherent transmission media comprising the soft healthybiological tissue (38G) comprises particles which comprise electricallycharged particles, and comprise potential energy which changesinsignificantly relative to the potential energy comprised by respectivesurroundings and the total energy comprised by coherently transmittedelectromagnetically neutralized wave-particle behaving entities.Wherein, coherent transmission processes involve a quantum mechanicalfunctional relation between the potential energy comprised by coherenttransmission media comprising the soft healthy biological tissue (38G)and the total energy comprised by coherently transmittedelectromagnetically neutralized wave-particle behaving entities.

During coherent transmission, the beam of electromagneticallyneutralized wave-particle behaving entities (4G) comprises waves whichproduce destructive interference to an extent, and respectivetime-varying electric and time-varying magnetic fields whichrespectively cancel to an extent. In effect, an amount of adverseelectromagnetic interaction of the beam of electromagneticallyneutralized wave-particle behaving entities (4G) with electricallycharged particles comprised in soft healthy biological tissue (38G) iseliminated in direct proportion to the time-average electric fluxdensity which is eliminated from the beam of electromagneticallyneutralized wave-particle behaving entities (4G). (Note, if a beam ofpartly electromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities is applied, then therespectively applied beam of partly electromagnetically neutralized andpartly electromagnetically functional wave-particle behaving entitiescan electromagnetically interact with electrically charged particlescomprised in the coherent transmission media (comprising soft healthybiological tissue) in direct proportion to the time-average electricflux density comprised in the beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities respectively applied. Also, note that here a filter isapplied to remove unwanted electromagnetically functional wave-particlebehaving entities (by way of electromagnetic interaction) from the beamof electromagnetically neutralized wave-particle behaving entitiesapplied to prevent unwanted adverse electromagnetic interaction ofelectromagnetically functional wave-particle behaving entities in thebeam of electromagnetically neutralized wave-particle behaving entitiesapplied (due to systematic and/or random error) with electricallycharged particles comprised in the coherently transmitting soft healthybiological tissue. Wherein, the radiation absorbed dose (RAD) of softhealthy biological tissue would be decreased to an extent, and thusadverse electromagnetic effects of radiological treatment would beeliminated to an extent (e.g., the destruction of soft healthybiological tissue would be eliminated to an extent.);

Step 3) the beam of electromagnetically neutralized wave-particlebehaving entities (4G) is incoherently scattered to an extent bypotential-energy-type and electromagnetic-type incoherently scatteringmedia comprised in the hard treatment site (8G) so to produce a beam ofelectromagnetically functional wave-particle behaving entities (40G)which comprises electromagnetically functional wave-particle behavingentities produced by incoherent scattering comprising waves whichcomprise random relative phase relations which neither superimpose norproduce interference, such that associated electric and magnetic fieldintensities respectively add so to produce a non-zero magnitude oftime-average electric flux density comprised in the hard treatment site(8G) (or also the beam of electromagnetically functional wave-particlebehaving entities (40G) produced can comprise electromagneticallyfunctional wave-particle behaving entities comprised by any remainingportion of a beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities which isnot incoherently scattered if a beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities is applied).

In this case, potential-energy-type incoherently scattering mediacomprises an irregularly ordered distribution of irregularly shapedparticles which each comprise: a) potential energy which changessignificantly relative to the potential energy comprised by respectivesurroundings and the total energy comprised by incoherently scatteredwave-particle behaving entities; and

b) a size and spacing which are each comparable to, or significantlylarger than, the wavelength of the waves comprised by respectivewave-particle behaving entities incoherently scattered from the beam ofelectromagnetically neutralized wave-particle behaving entities (4G).Wherein, potential-energy-type incoherent scattering processes (e.g.,irregular reflections and/or irregular refractions) involve a quantummechanical functional relation between the potential energy comprised bythe hard treatment site (8G) comprising the potential-energy-typeincoherently scattering media and the total energy comprised byincoherently scattered wave-particle behaving entities.

Also, in step 3), electromagnetic-type incoherently scattering mediacomprise an irregularly ordered distribution of electrically chargedparticles (e.g., atoms and molecules) which each comprise spacing whichis comparable to, or significantly larger than, the wavelength of thewaves comprised by the respective incoherently scatteredelectromagnetically functional wave-particle behaving entities. Wherein,electromagnetic-type incoherent scattering processes (e.g., incoherentCompton scattering) involve electromagnetic interaction. (Note, if abeam of totally electromagnetically neutralized wave-particle behavingentities is applied in the preferred embodiment in FIG. (31), thenelectromagnetic-type incoherent scattering of electromagneticallyfunctional wave-particle behaving entities by electromagnetic-typeincoherently scattering media would occur dependent upon the onset ofthe production of the electromagnetically functional wave-particlebehaving entities by potential-energy-type incoherent scattering.However, if a beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities isapplied in the preferred embodiment in FIG. (31), thenelectromagnetic-type incoherent scattering of electromagneticallyfunctional wave-particle behaving entities by electromagnetic-typeincoherently scattering media would occur independent of the onset ofthe production of the electromagnetically functional wave-particlebehaving entities by potential-energy-type incoherent scattering, sincea beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities alreadycomprises wave-particle behaving entities which are partlyelectromagnetically functional.)

Furthermore, in step 3), transmission media comprised in the hardtreatment site (8G) transmit an extent of such a beam ofelectromagnetically functional wave-particle behaving entitiescomprising electromagnetically functional wave-particle behavingentities produced by incoherent scattering (or also comprising anyremaining portion of a beam of partly electromagnetically neutralizedand partly electromagnetically functional wave-particle behavingentities which is not incoherently scattered if a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities is applied) toelectromagnetic-type utilizing media, which comprise electricallycharged particles, comprised in the hard treatment site (8G). (Note,transmission media comprised in incoherent scattering and transmittingmedia requires any parameters with respective values which wouldeffectively transmit the type of respectively transmitted wave-particlebehaving entities applied including those parameters comprised byincoherently scattering media comprised in the incoherently scatteringand transmitting media respectively applied.);

Step 4) an extent of the transmitted electromagnetically functionalwave-particle behaving entities produced by incoherent scattering (oralso an extent of any transmitted remaining portion of a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities if a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities is applied) are utilized byway of electromagnetic interaction by electromagnetic-type utilizingmedia comprising electrically charged particles comprised in the hardtreatment site (8G) so to produce ionization or also dissociation of thehard treatment site (8G), and thus produce the result of the respectivepreferred embodiment.

Here, ionization processes comprise photoionization, Compton scattering,electron and positron pair production, or also secondary (etc.)incoherent scattering. Nevertheless, such ionization processes involveelectromagnetic interaction. (Note, if a beam of electromagneticallyneutralized wave-particle behaving electrons is applied, thenelectromagnetically functional wave-particle behaving electrons whichare transmitted to the treatment site and subsequently become staticwill then be electromagnetically functional electrons which caneffectively produce a form of ionization of the treatment site. Also,note that an extent of the electrically charged particles surrounding atreatment site might adversely electromagnetically interact withtransmitted electromagnetically functional wave-particle behavingentities so to produce adverse electromagnetic effects due to thelimitations of the localization of the beam of electromagneticallyfunctional wave-particle behaving entities produced by incoherentscattering in a treatment site in such preferred embodiments of thepresent invention as the preferred embodiment herein.)

FIG. (32) shows a somewhat more specific preferred embodiment which isapplied for performing radiological treatment in an effective manner.The steps applied in the preferred embodiment in FIG. (31) are ingeneral applied in the preferred embodiment in FIG. (32) except that thepreferred embodiment in FIG. (32) more exclusively applies a focusedbeam of electromagnetically neutralized wave-particle behaving entitiesfor radiological treatment.

In the preferred embodiment in FIG. (32), apparatus (which is isolatedfrom mechanical vibrations), more specifically, produces a focused beamof electromagnetically neutralized wave-particle behaving entities whichis coherently transmitted by coherent transmission media comprising afilter, air, and soft healthy biological tissue towards a hard treatmentsite (rectangular block comprising the dashed line format) (e.g., acalcified tumor or pathological bone), such that adverse electromagneticinteraction of the beam of electromagnetically neutralized wave-particlebehaving entities with electrically charged particles comprised in thecoherent transmission media (comprising soft healthy biological tissue)is eliminated to an extent. Wherein, the adverse electromagnetic effectsof transmitting energy for radiological treatment are eliminated to anextent.

Then, the coherently transmitted beam of electromagnetically neutralizedwave-particle behaving entities is incoherently scattered to an extentby incoherently scattering media comprised in the hard treatment site soto produce a beam of electromagnetically functional wave-particlebehaving entities (which comprises a non-zero magnitude of time-averageelectric flux density) in the treatment site (i.e., a beam ofelectromagnetically functional wave-particle behaving entities isproduced comprising electromagnetically functional wave-particlebehaving entities produced by incoherent scattering or also comprisingany remaining portion of a beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities which is not incoherently scattered if a beam ofpartly electromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities is applied). Also, in thisstep, an extent of such a beam of electromagnetically functionalwave-particle behaving entities produced is transmitted by transmissionmedia comprised in the hard treatment site to electromagnetic-typeutilizing media comprised in the hard treatment site. Lastly, an extentof the transmitted electromagnetically functional wave-particle behavingentities produced by incoherent scattering (or also an extent of anytransmitted remaining portion of a beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities if a beam of partly electromagnetically neutralizedand partly electromagnetically functional wave-particle behavingentities is applied) are utilized by way of electromagnetic interactionby electromagnetic-type utilizing media comprising electrically chargedparticles comprised in the treatment site so to produce ionization oralso dissociation of the hard treatment site, and thus produce theresult of the respective preferred embodiment.

FIG. (33) shows another somewhat more specific preferred embodimentwhich is applied for performing radiological treatment in an effectivemanner. The steps applied in the preferred embodiment in FIG. (18) are,in general, applied in the preferred embodiment in FIG. (33) hereinexcept that the preferred embodiment herein applies a focused beam ofelectromagnetically neutralized wave-particle behaving entities and thetarget (rectangle shown in a dashed line format) comprises, morespecifically, a hard media, which comprises incoherently scatteringmedia, transmission media, and electrically charged particles which mayor may not be part of the treatment site; while, necessarily, thetreatment site of radiological treatment is a soft treatment sitelocated posterior to (beyond) the hard media.

Wherein, in the preferred embodiment in FIG. (33), apparatus (which isisolated from mechanical vibrations) produces a focused beam ofelectromagnetically neutralized wave-particle behaving entities which iscoherently transmitted by coherent transmission media comprising afilter, air, and soft healthy biological tissue to the hard mediatowards a focus in the soft treatment site located posterior to the hardmedia, such that adverse electromagnetic interaction of the beam ofelectromagnetically neutralized wave-particle behaving entities withelectrically charged particles comprised in the coherent transmissionmedia (comprising soft healthy biological tissue) is eliminated to anextent. Wherein, the adverse electromagnetic effects of transmittingenergy for radiological treatment are eliminated to an extent.

Then, the coherently transmitted beam of electromagnetically neutralizedwave-particle behaving entities is incoherently scattered to an extentby incoherently scattering media comprised in the hard media so toproduce a beam of electromagnetically functional wave-particle behavingentities (which comprises a non-zero magnitude of time-average electricflux density) in the hard media (i.e., a beam of electromagneticallyfunctional wave-particle behaving entities is produced comprisingelectromagnetically functional wave-particle behaving entities producedby incoherent scattering or also comprising any remaining portion of abeam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities which isnot incoherently scattered if a beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities is applied).

Also, in this step, an extent of such a beam of electromagneticallyfunctional wave-particle behaving entities produced is transmitted bytransmission media comprised in the hard media, and comprised in thesoft treatment site located posteriorly, to the hard media comprisingelectrically charged particles and to electromagnetic-type utilizingmedia comprising electrically charged particles comprised in the softtreatment site located posteriorly.

Then, an extent of the transmitted beam of electromagneticallyfunctional wave-particle behaving entities (or also an extent of anytransmitted remaining portion of a beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities if a beam of partly electromagnetically neutralizedand partly electromagnetically functional wave-particle behavingentities is applied) is utilized by way of electromagnetic interactionby electromagnetic-type utilizing media comprising electrically chargedparticles comprised in the soft treatment site so to produce ionizationor also dissociation of the soft treatment site, and either utilized bymedia comprising electrically charged particles comprised in the hardmedia located anteriorly by way of electromagnetic interaction so toproduce ionization or also dissociation of the hard media when the hardmedia is part of the overall treatment site, or adversely absorbed byway of electromagnetic interaction by electrically charged particlescomprised in the hard media located anteriorly when the hard media isnot part of the overall treatment site so to hinder the accomplishmentof the objective of the respective application of the present invention.

FIG. (34) shows another somewhat more specific preferred embodimentwhich is applied for radiological treatment in an effective manner. Thesteps applied in the preferred embodiment in FIG. (32) are, in general,applied in the preferred embodiment in FIG. (34). However, the preferredembodiment in FIG. (34) applies more specific steps for radiologicaltreatment of a hard treatment site (e.g., a calcified tumor) which issurrounded by healthy brain tissue located in the brain of a surgicallyprepared patient who is supported by a steriotaxic device (showngenerically by a block drawing).

Wherein, in the preferred embodiment in FIG. (34), more specifically,apparatus (which is isolated from mechanical vibrations) produces afocused beam of electromagnetically neutralized wave-particle behavingentities which is coherently transmitted by coherent transmission mediacomprising a filter, air, a surgically prepared hole in the skull of thepatent, and soft healthy brain tissue towards a focus in the hardtreatment site, such that adverse electromagnetic interaction of thebeam of electromagnetically neutralized wave-particle behaving entitieswith electrically charged particles comprised in the coherenttransmission media (comprising soft healthy brain tissue comprised intissue surrounding the hard treatment site) is eliminated to an extent.Wherein, the adverse electromagnetic effects of transmitting energy forradiological treatment are eliminated to an extent.

Then, the beam of electromagnetically neutralized wave-particle behavingentities is incoherently scattered to an extent by incoherentlyscattering media comprised in the hard treatment site so to produce abeam of electromagnetically functional wave-particle behaving entities(which comprises a non-zero magnitude of time-average electric fluxdensity) (not shown) in the hard treatment site (i.e., a beam ofelectromagnetically functional wave-particle behaving entities isproduced comprising electromagnetically functional wave-particlebehaving entities produced by incoherent scattering or also comprisingany remaining portion of a beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities which is not incoherently scattered if a beam ofpartly electromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities is applied).

Also, in this step, an extent of such a beam of electromagneticallyfunctional wave-particle behaving entities produced is transmitted bytransmission media comprised in the hard treatment site toelectromagnetic-type utilizing media comprising electrically chargedparticles comprised in the hard treatment site. Lastly, an extent of thetransmitted electromagnetically functional wave-particle behavingentities produced by incoherent scattering (or also an extent of anytransmitted remaining portion of a beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities if a beam of partly electromagnetically neutralizedand partly electromagnetically functional wave-particle behavingentities is applied) are utilized by way of electromagnetic interactionby electromagnetic-type utilizing media comprising electrically chargedparticles comprised in the hard treatment site so to produce ionizationor also dissociation of the hard treatment site, and thus produce theresult of the respective preferred embodiment.

FIG. (34A) is an enlarged view of a section of the preferred embodimentfor radiological treatment shown in FIG. (34) and exclusively shows, inthe patient's brain, the beam of electromagnetically neutralizedwave-particle behaving entities in an area of the healthy soft braintissue and projecting into the hard treatment site, and shows the beamof electromagnetically functional wave-particle behaving entitiesrespectively produced in the hard treatment site.

FIG. (35) shows another somewhat more specific preferred embodimentwhich is applied for radiological treatment in an effective manner. Thepreferred embodiment in FIG. (35), in general, applies the steps appliedin the preferred embodiment in FIG. (33), yet, more specifically, isapplied for radiological treatment of a soft treatment site (e.g., asoft organic tumor) which is located posterior to hard media, whichcomprises incoherently scattering media, transmission media, andelectrically charged particles, which may or may not be part of thetreatment site, while, necessarily, the treatment site is the softtreatment site located posterior to (beyond) the hard media, and which,along with the soft treatment site, is surrounded by tissue comprisingsoft healthy brain tissue located in the brain of a surgically preparedpatient who is supported by a steriotaxic device.

In the preferred embodiment in FIG. (35), apparatus produces a beam ofelectromagnetically neutralized wave-particle behaving entities which istransmitted by coherent transmission media comprising a filter, air, asurgically prepared hole in the skull of the patent, and soft healthybrain tissue to the hard media located anterior to the soft treatmentsite, such that adverse electromagnetic interaction of the beam ofelectromagnetically neutralized wave-particle behaving entities withelectrically charged particles comprised in the coherent transmissionmedia (comprising soft healthy brain tissue) is eliminated to an extent.Wherein, the adverse electromagnetic effects of transmitting energy forradiological treatment are eliminated to an extent.

Then, the beam of electromagnetically neutralized wave-particle behavingentities is incoherently scattered to an extent by incoherentlyscattering media (comprised in the hard media which is located anteriorto the soft treatment site) so to produce a beam of electromagneticallyfunctional wave-particle behaving entities (which comprises a non-zeromagnitude of time-average electric flux density) (not shown) in the hardmedia (i.e., a beam of electromagnetically functional wave-particlebehaving entities is produced comprising electromagnetically functionalwave-particle behaving entities produced by incoherent scattering oralso comprising any remaining portion of a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities which is not incoherentlyscattered if a beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities isapplied).

Also, in this step, transmission media comprised in the hard media, andcomprised in the soft treatment site located posteriorly, transmit anextent of such a beam of electromagnetically functional wave-particlebehaving entities produced to the hard media comprising electricallycharged particles and to electromagnetic-type utilizing media comprisingelectrically charged particles comprised in the soft treatment sitelocated posteriorly.

Then, an extent of the transmitted beam of electromagneticallyfunctional wave-particle behaving entities (i.e., an extent of thetransmitted beam of electromagnetically functional wave-particlebehaving entities comprising electromagnetically functionalwave-particle behaving entities produced by incoherent scattering oralso an extent of any transmitted remaining portion of a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities if a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities is applied) is utilized byway of electromagnetic interaction by electromagnetic-type utilizingmedia comprising electrically charged particles comprised in the softtreatment site so to produce ionization or also dissociation of the softtreatment site, and either utilized by way of electromagneticinteraction by media comprising electrically charged particles comprisedin the hard media located anteriorly so to produce ionization or alsodissociation of the hard media when the hard media (e.g., a calcifiedtumor) is part of the overall treatment site, or adversely absorbed byway of electromagnetic interaction by electrically charged particlescomprised in the hard media located anteriorly when the hard media isnot part of the overall treatment site so to hinder the accomplishmentof the objective of the respective application of the present invention.

FIG. (35A) is an enlarged view of a section of the preferred embodimentfor radiological treatment shown in FIG. (35) and exclusively shows, inthe patient's brain, the beam of electromagnetically neutralizedwave-particle behaving entities in an area of the soft healthy braintissue and projecting into the hard media, and shows the beam ofelectromagnetically functional wave-particle behaving entitiesrespectively produced in the hard media and in the soft treatment sitewhich is located posterior to the hard media.

FIG. (36) shows another preferred embodiment which is applied forradiological treatment in an effective manner. The steps applied in thepreferred embodiment in FIG. (32) are applied in the preferredembodiment in FIG. (36) except that the treatment site is comprised in abone.

Wherein, in the preferred embodiment in FIG. (36), apparatus (which isisolated from mechanical vibrations) produces a beam ofelectromagnetically neutralized wave-particle behaving entities which iscoherently transmitted by coherent transmission media comprising afilter, air, and soft healthy biological tissue located anterior to abone, such that adverse electromagnetic interaction of the beam ofelectromagnetically neutralized wave-particle behaving entities withelectrically charged particles comprised in the coherent transmissionmedia (comprising soft healthy biological tissue) is eliminated to anextent. Wherein, the adverse electromagnetic effects of transmittingenergy for radiological treatment are eliminated to an extent.

Then, the coherently transmitted beam of electromagnetically neutralizedwave-particle behaving entities is incoherently scattered to an extentby incoherently scattering media in the bone so to produce a beam ofelectromagnetically functional wave-particle behaving entities(comprising a non-zero magnitude of time-average electric flux density)in the bone (i.e., a beam of electromagnetically functionalwave-particle behaving entities is produced comprisingelectromagnetically functional wave-particle behaving entities producedby incoherent scattering or also comprising any remaining portion of abeam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities which isnot incoherently scattered if a beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities is applied).

Also, in this step, transmission media in the bone transmit an extent ofsuch a beam of electromagnetically functional wave-particle behavingentities produced to electromagnetic-type utilizing media comprisingelectrically charged particles comprised in the bone. Lastly, an extentof the transmitted electromagnetically functional wave-particle behavingentities produced by incoherent scattering (or also an extent of anytransmitted remaining portion of a beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities if a beam of partly electromagnetically neutralizedand partly electromagnetically functional wave-particle behavingentities is applied) are utilized by way of electromagnetic interactionby electromagnetic-type utilizing media comprising electrically chargedparticles comprised in the bone so to produce so to produce ionizationof the bone, and thus produce the result of the respective preferredembodiment.

FIG. (37) shows another preferred embodiment which is applied forradiological treatment in an effective manner. The steps applied in thepreferred embodiment in FIG. (33) are, in general, applied in thepreferred embodiment in FIG. (37). However, more specifically, in thepreferred embodiment in FIG. (37), the target (rectangle shown in adashed line format) is comprised in a bone which comprises hardincoherently scattering media comprising electrically charged particleswhich may or may not be part of the treatment site; while, necessarily,the treatment site is a soft treatment site comprised in the bone marrowlocated posterior to (beyond) the given bone.

Wherein, in the preferred embodiment in FIG. (37), apparatus produces abeam of electromagnetically neutralized wave-particle behaving entitieswhich is coherently transmitted by coherent transmission mediacomprising a filter, air, and soft healthy biological tissue to the bone(which is located anterior to the soft treatment site comprised in therespective bone marrow), such that adverse electromagnetic interactionof the beam of electromagnetically neutralized wave-particle behavingentities with electrically charged particles comprised in the coherenttransmission media (comprising soft healthy biological tissue) iseliminated to an extent. Wherein, the adverse electromagnetic effects oftransmitting energy for radiological treatment are eliminated to anextent.

Then, the coherently transmitted beam of electromagnetically neutralizedwave-particle behaving entities is incoherently scattered to an extentby incoherently scattering media comprised in the bone so to produce abeam of electromagnetically functional wave-particle behaving entities(comprising a non-zero magnitude of time-average electric flux density)(i.e., a beam of electromagnetically functional wave-particle behavingentities is produced comprising electromagnetically functionalwave-particle behaving entities produced by incoherent scattering oralso comprising any remaining portion of a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities which is not incoherentlyscattered if a beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities isapplied). Also, in this step, transmission media in the bone and in thebone marrow (located posteriorly) transmit an extent of such a beam ofelectromagnetically functional wave-particle behaving entities producedto the bone, which comprises electrically charged particles, and toelectromagnetic-type utilizing media comprising electrically chargedparticles comprised in the bone marrow located posteriorly.

Subsequently, an extent of such a transmitted beam ofelectromagnetically functional wave-particle behaving entities isutilized by way of electromagnetic interaction by electromagnetic-typeutilizing media comprising electrically charged particles comprised inthe bone marrow so to produce ionization of the bone marrow, and eitherutilized by way of electromagnetic interaction by media comprisingelectrically charged particles comprised in the bone located anteriorlyso to produce ionization of the bone when the bone is part of theoverall treatment site, or adversely absorbed by way of electromagneticinteraction by electrically charged particles comprised in the bonelocated anteriorly when the bone is not part of the overall treatmentsite so to hinder the accomplishment of the objective of the respectiveapplication of the present invention.

FIG. (38) shows a preferred embodiment which is applied for performingradiotherapy in an effective manner. The steps applied in the preferredembodiment in FIG. (31) are applied in the preferred embodiment in FIG.(38) except that the beam of electromagnetically neutralizedwave-particle behaving entities is broad and the hard treatment site islarger.

FIG. (39) shows another preferred embodiment which is applied forperforming radiotherapy in an effective manner. The method referred toin the preferred embodiment in FIG. (38) is basically applied in thepreferred embodiment in FIG. (39) with some modifications including thatthe beam of electromagnetically neutralized wave-particle behavingentities is broad and the treatment site comprises a plurality of hardtreatment sites.

In the preferred embodiment in FIG. (39), apparatus (which is isolatedfrom mechanical vibrations) produces a broad beam of electromagneticallyneutralized wave-particle behaving entities, an extent of which iscoherently transmitted by coherent transmission media comprising afilter, air, and soft healthy biological tissue to the hard treatmentsites comprising the plurality of hard treatment sites, and an extent ofwhich is coherently transmitted by coherent transmission mediacomprising a filter, air, and soft healthy biological tissue through thebiological specimen to a shielding apparatus, such that adverseelectromagnetic interaction of the beam of electromagneticallyneutralized wave-particle behaving entities with electrically chargedparticles comprised in the coherent transmission media (comprising thesoft healthy biological tissue) is eliminated to an extent. Wherein, theadverse electromagnetic effects of transmitting energy for radiotherapyare eliminated to an extent.

Then, the beam portion of electromagnetically neutralized wave-particlebehaving entities which is coherently transmitted to the plurality ofhard treatment sites is incoherently scattered by incoherentlyscattering media comprised in the respective hard treatment sites toproduce electromagnetically functional wave-particle behaving entities(comprising a non-zero magnitude of time-average electric flux density)in the respective hard treatment sites (i.e., in each respective hardtreatment site, a beam of electromagnetically functional wave-particlebehaving entities is produced comprising electromagnetically functionalwave-particle behaving entities produced by incoherent scattering oralso comprising any remaining portion of a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities which is not incoherentlyscattered if a beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities isapplied). Also, in this step, transmission media in each hard treatmentsite transmits an extent of the beam of electromagnetically functionalwave-particle behaving entities produced in each respective treatmentsite to electromagnetic-type utilizing media comprising electricallycharged particles comprised in the respective hard treatment sites.

Lastly, an extent of the transmitted electromagnetically functionalwave-particle behaving entities produced by incoherent scattering (oralso an extent of any transmitted remaining portion of a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities if a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities is applied) is utilized byway of electromagnetic interaction by electromagnetic-type utilizingmedia comprising electrically charged particles comprised in eachrespective hard treatment site so to produce ionization of eachrespective hard treatment site, and thus produce the result of therespective preferred embodiment.

However, the portion of the beam of electromagnetically neutralizedwave-particle behaving entities which is coherently transmitted throughthe biological specimen to the shielding apparatus can be incoherentlyscattered by incoherently scattering apparatus comprised by theshielding apparatus, such that electromagnetically functionalelectromagnetic field quanta (comprising a non-zero time-averageelectric flux density), which are produced by incoherent scattering inthe shielding apparatus, would be transmitted by transmitting mediacomprised in the shielding apparatus to, and then absorbed by,electromagnetically absorptive media comprised by the shieldingapparatus; or also any electromagnetically functional wave-particlebehaving entities produced by incoherent scattering, or also anyremaining portion of a beam of partly electromagnetically neutralizedand partly electromagnetically functional electromagnetic field quantawhich is not incoherently scattered, if a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional electromagnetic field quanta is applied, which aretransmitted through the biological specimen to the shielding apparatuscan be absorbed, or incoherently scattered by incoherently scatteringapparatus, and transmitted by transmitting apparatus to, and thenabsorbed by, electromagnetically absorptive apparatus comprisingelectrically charged particles comprised in the shielding apparatus.

FIG. (40) shows another generalized preferred embodiment which isapplied for radiological treatment in an effective manner. The stepsapplied in the preferred embodiment in FIG. (21) are, in general,applied in the preferred embodiment in FIG. (40) with somemodifications.

In the preferred embodiment in FIG. (40), apparatus (which is isolatedfrom mechanical vibrations) produces a focused beam ofelectromagnetically neutralized wave-particle behaving electrons ofsufficiently high energy (i.e., non-refracting electrons), which iscontinuous or pulsed, and which comprises electromagneticallyneutralized wave-particle behaving electrons which individually andcollectively comprise potential energy so to effectively produce apotential-energy-type incoherent scattering (and transmitting) medium atthe focus; or also an electromagnetic-type (i.e., an electrostatic-type)incoherent scattering medium at the focus due to electron repulsion if afocused beam of partly electromagnetically neutralized and partlyelectromagnetically functional electrically charged electrons isapplied. The focused beam of electromagnetically neutralizedwave-particle behaving electrons is coherently transmitted by coherenttransmission media comprising filter, air, and soft healthy biologicaltissue to the focus of the beam of electromagnetically neutralizedwave-particle behaving electrons in the soft treatment site (rectangularblock comprising the dashed line format) (e.g., an organic tumor), suchthat adverse electromagnetic interaction of the beam ofelectromagnetically neutralized wave-particle behaving electrons withelectrically charged particles comprised in the coherent transmissionmedia (comprising soft healthy biological tissue) is eliminated to anextent. Wherein, the adverse electromagnetic effects of transmittingenergy for radiological treatment are eliminated to an extent (e.g., thedestruction of soft healthy biological tissue in radiological treatmentis eliminated to an extent by decreasing the radiation absorbed dose(RAD) of the respective soft healthy biological tissue).

Then, the coherently transmitted beam of wave-particle behavingelectrons is incoherently scattered to an extent by incoherentlyscattering media (comprised by the focus of the beam ofelectromagnetically neutralized wave-particle behaving electrons) so toproduce a beam of electromagnetically functional wave-particle behavingelectrons (comprising a non-zero magnitude of time-average electric fluxdensity) in the soft treatment site (i.e., a beam of electromagneticallyfunctional wave-particle behaving entities is produced comprisingelectromagnetically functional wave-particle behaving entities producedby incoherent scattering or also comprising any remaining portion of abeam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities which isnot incoherently scattered if a beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities is applied). Also, in this step, an extent of such abeam of electromagnetically functional wave-particle behaving electronsproduced is transmitted by transmission media comprised in the softtreatment site to electromagnetic-type utilizing media comprisingelectrically charged particles comprised in the soft treatment site.Lastly, an extent of the transmitted electromagnetically functionalwave-particle behaving electrons produced by incoherent scattering (oralso an extent of any transmitted remaining portion of a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving electrons if a focused beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving electrons is applied) are utilized byway of electromagnetic interaction by electromagnetic-type utilizingmedia comprising electrically charged particles comprised in the softtreatment site so to produce ionization or also dissociation of the softtreatment site, and thus produce the result of the respective preferredembodiment.

FIG. (41) shows another somewhat more specific preferred embodimentwhich is applied for radiological treatment in an effective manner. Thesteps applied in the preferred embodiment in FIG. (40) are, in general,applied in the preferred embodiment in FIG. (41). However, the preferredembodiment in FIG. (41) applies more specific steps for radiologicaltreatment of a soft treatment site (e.g., an organic tumor) which issurrounded by soft healthy brain tissue located in the brain of asurgically prepared patient who is supported by a steriotaxic device(shown generically by a block drawing).

Wherein, in the preferred embodiment in FIG. (41), more specifically,apparatus (which is isolated from mechanical vibrations) produces afocused beam of electromagnetically neutralized wave-particle behavingelectrons of sufficiently high energy (i.e., non-refracting electrons)which individually and collectively comprise potential energy. Then, thebeam of electromagnetically neutralized wave-particle behaving electronsis coherently transmitted by coherent transmission media comprising afilter, air, a surgically prepared hole in the skull of the patent, andsoft healthy brain tissue to the focus of the beam ofelectromagnetically neutralized wave-particle behaving electrons, suchthat adverse electromagnetic interaction of the beam ofelectromagnetically neutralized wave-particle behaving electrons withelectrically charged particles comprised in the coherent transmissionmedia (comprising soft healthy brain tissue) is eliminated to an extent.Wherein, the adverse electromagnetic effects of transmitting energy forradiological treatment are eliminated to an extent (e.g., thedestruction of soft healthy biological tissue in radiological treatmentis eliminated to an extent by decreasing the radiation absorbed dose(RAD) of the respective soft healthy biological tissue).

Then, the coherently transmitted beam of electromagnetically neutralizedwave-particle behaving electrons is incoherently scattered to an extentby incoherently scattering media at the focus of the beam ofelectromagnetically neutralized wave-particle behaving electrons so toproduce a beam of electromagnetically functional wave-particle behavingelectrons (comprising a non-zero magnitude of time-average electric fluxdensity) in the soft treatment site (i.e., a beam of electromagneticallyfunctional wave-particle behaving electrons is produced comprisingelectromagnetically functional wave-particle behaving electrons producedby incoherent scattering or also comprising any remaining portion of abeam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving electrons which isnot incoherently scattered if a beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving electrons is applied).

Here, the focus of the beam of electromagnetically neutralizedwave-particle behaving electrons produces a potential-energy-typeincoherent scattering (and transmitting) medium at the focus; or also anelectromagnetic-type (i.e., an electrostatic-type) incoherent scatteringmedium at the focus due to electron repulsion if a focused beam ofpartly electromagnetically neutralized and partly electromagneticallyfunctional electrically charged electrons is applied.

Also, in this step, transmission media in the soft treatment sitetransmit an extent of the electromagnetically functional wave-particlebehaving electrons produced by incoherent scattering (or also transmitan extent of any remaining portion of a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving electrons if a focused beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving electrons is applied) toelectromagnetic-type utilizing media comprising electrically chargedparticles comprised in the soft treatment site. Lastly, an extent of thetransmitted electromagnetically functional wave-particle behavingelectrons produced by incoherent scattering (or also an extent of anyremaining portion of a beam of partly electromagnetically neutralizedand partly electromagnetically functional wave-particle behavingelectrons if a focused beam of partly electromagnetically neutralizedand partly electromagnetically functional wave-particle behavingelectrons is applied) are utilized by way of electromagnetic interactionby electromagnetic-type utilizing media comprising electrically chargedparticles comprised in the soft treatment site so to produce ionizationor also dissociation of the soft treatment site, and thus produce theresult of the respective preferred embodiment.

FIG. (41A) is an enlarged view of a section of the preferred embodimentfor radiological treatment shown in FIG. (41) and exclusively shows, inthe patient's brain, the beam of electromagnetically neutralizedwave-particle behaving electrons in an area of the soft healthy braintissue and shows the beam of electromagnetically functionalwave-particle behaving electrons respectively produced in the softtreatment site.

FIG. (42) shows a plan side view of a somewhat narrowly scoped andgeneralized preferred embodiment of the present invention which isapplied for performing non-invasive ophthalmic surgery in an effectivemanner. In this case, the embodiment in FIG. (42) eliminates an extentof the adverse electromagnetic interaction (e.g., Rayleigh scatteringand resonance absorption) of electromagnetic field quanta (e.g., opticalwavelength electromagnetic field quanta) with healthy ocular media innon-invasive ophthalmic surgery, hence eliminating an extent of theadverse electromagnetic effects of transmitting energy for non-invasiveophthalmic surgery (e.g., hence eliminating an extent of the destructionof healthy ocular media, such as, eliminating an extent of theopacification of clear ocular media located anterior to the retinaand/or eliminating an extent of the destruction of healthy retinaltissue in non-invasive ophthalmic surgery).

The steps applied in the preferred embodiment in FIG. (20) are, ingeneral, applied in the preferred embodiment in FIG. (42). However, morespecifically, the preferred embodiment in FIG. (42) is applied fornon-invasive ophthalmic surgery as follows:

Step 1) apparatus (2H) (which is isolated from mechanical vibrations)produces a beam of partly electromagnetically neutralized and partlyelectromagnetically functional surgical wavelength electromagnetic fieldquanta (4H);

Step 2) the beam of partly electromagnetically neutralized and partlyelectromagnetically functional electromagnetic field quanta (4H) iscoherently transmitted by coherent transmission media to an ophthalmictreatment site (8H). Wherein, coherent transmission media comprise thefilter (34H), the air (36H), healthy ocular media (38H) (e.g.,comprising, clear corneal tissue, clear aqueous humor, clear ocularlens, clear vitreous humor, or also clear retinal tissue).

Here, during coherent transmission, adverse electromagnetic interactionof the beam of partly electromagnetically neutralized and partlyelectromagnetically functional electromagnetic field quanta withelectrically charged particles comprised in the coherent transmissionmedia is eliminated to an extent (e.g., Rayleigh scattering andrespective beam broadening, and resonance absorption and respectiveheating of healthy ocular media can be eliminated to an extent).Wherein, the adverse electromagnetic effects of transmitting energy fornon-invasive ophthalmic surgery are eliminated to an extent (e.g.,opacification of clear ocular media located anterior to the treatmentsite or also the destruction of healthy retinal tissue surrounding thetreatment site can be eliminated to an extent). (Note, the respectivelyapplied beam of partly electromagnetically neutralized and partlyelectromagnetically functional electromagnetic field quanta canadversely electromagnetically interact with electrically chargedparticles comprised in the coherent transmission media in directproportion to the time-average electric flux density comprised by therespectively applied beam of partly electromagnetically neutralized andpartly electromagnetically functional electromagnetic field quanta.Also, note that herein a filter is applied to remove unwantedelectromagnetically functional electromagnetic field quanta from thebeam of partly electromagnetically neutralized and partlyelectromagnetically functional electromagnetic field quanta applied (byway of electromagnetic interaction) to prevent unwanted adverseelectromagnetic interaction of electromagnetically functionalelectromagnetic field quanta in the beam of partly electromagneticallyneutralized and partly electromagnetically functional electromagneticfield quanta (produced by systematic and/or random error) withelectrically charged particles comprised in healthy ocular media so todecrease the adverse electromagnetic effects in non-invasive ophthalmicsurgery (e.g., so to decrease the opacification of clear ocular mediaand decrease the destruction of healthy retinal tissue)).

Herein, coherently transmitting healthy ocular media (38H) comprisesparticles, which comprise electrically charged particles, and eachcomprise: a) potential energy which changes insignificantly relative tothe potential energy comprised by respective surroundings and the totalenergy comprised by coherently transmitted partly electromagneticallyneutralized and partly electromagnetically functional electromagneticfield quanta; and b) spacing or also a size which are each significantlysmaller than the wavelength of the waves comprised in the coherentlytransmitted beam of partly electromagnetically neutralized and partlyelectromagnetically functional electromagnetic field quanta (4H). Inthis case, coherent transmission processes involve a quantum mechanicalfunctional relation between the potential energy comprised by coherentlytransmitting healthy ocular media and the total energy comprised bycoherently transmitted partly electromagnetically neutralized and partlyelectromagnetically functional electromagnetic field quanta; andcoherent transmission processes also involve electromagneticinteraction;

Step 3), the beam of partly electromagnetically neutralized and partlyelectromagnetically functional electromagnetic field quanta (4H) isincoherently scattered to an extent by potential-energy-type andelectromagnetic-type incoherently scattering media comprised in theophthalmic treatment site (8H) (e.g., incoherently scattering mediacomprise abnormal ocular opacifications, retinal pigmented epithelium,choroidal tissue, and/or scleral tissue) so to produce the beam ofelectromagnetically functional electromagnetic field quanta (40H) whichcomprises incoherently scattered electromagnetically functionalelectromagnetic field quanta which comprise randomly distributed waveswhich comprise random relative phase relations and neither superimposenor produce interference, such that associated electric and magneticfield intensities respectively add in beam (40H) so to produce arespective non-zero magnitude of time-average electric flux density inthe ophthalmic treatment site (8H) (or also the beam ofelectromagnetically functional electromagnetic field quanta produced cancomprise electromagnetically functional electromagnetic field quantacomprising any remaining portion of a beam of partly electromagneticallyneutralized and partly electromagnetically functional electromagneticfield quanta which is not incoherently scattered from the beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional electromagnetic field quanta applied).

In this case, potential-energy-type incoherently scattering mediacomprises an irregularly ordered distribution of irregularly shapedparticles which each comprise: a) potential energy which changessignificantly relative to the potential energy comprised by respectivesurroundings and the total energy comprised by incoherently scatteredelectromagnetic field quanta; and b) a size and spacing which are eachcomparable to, or significantly larger than, the wavelength of the wavescomprised by the respective electromagnetic field quanta incoherentlyscattered from beam (4H). Wherein, potential-energy-type incoherentscattering processes (e.g., irregular reflections and/or irregularrefractions) involve a quantum mechanical functional relation betweenthe potential energy comprised by the ophthalmic treatment site (8H)(comprising potential-energy-type incoherently scattering media) and thetotal energy comprised by respective electromagnetic field quantaincoherently scattered from beam (4H).

Also, in step 3), electromagnetic-type incoherently scattering mediacomprise an irregularly ordered distribution of electrically chargedparticles (e.g., atoms and molecules) which each comprise spacing whichis comparable to, or significantly larger than, the wavelength of thewaves comprised by the respective incoherently scattered electromagneticfield quanta. Wherein, electromagnetic-type incoherent scatteringprocesses (e.g., incoherent Rayleigh scattering) involve electromagneticinteraction. (Note, electromagnetic-type incoherent scattering ofelectromagnetically functional electromagnetic field quanta byelectromagnetic-type incoherently scattering media occurs independent ofthe onset of the production of the electromagnetically functionalelectromagnetic field quanta by potential-energy-type incoherentscattering, since a beam of partly electromagnetically neutralized andpartly electromagnetically functional electromagnetic field quantaalready comprises electromagnetic field quanta which are partlyelectromagnetically functional);

Furthermore, in step 3), transmission media comprised in the ophthalmictreatment site (8H) transmit an extent of the electromagneticallyfunctional electromagnetic field quanta produced by incoherentscattering (or also transmit an extent of any remaining portion of thebeam of partly electromagnetically neutralized and partlyelectromagnetically functional electromagnetic field quanta from thebeam of partly electromagnetically neutralized and partlyelectromagnetically functional electromagnetic field quanta applied) toelectromagnetic-type utilizing media comprised in the ophthalmictreatment site (8H). (Note, transmission media comprised in incoherentscattering and transmitting media would require any parameters withrespective values which would effectively transmit the type ofrespectively transmitted wave-particle behaving entities appliedincluding those parameters comprised by incoherently scattering mediacomprised in the incoherently scattering and transmitting mediarespectively applied; and,

Step 5) an extent of the transmitted electromagnetically functionalelectromagnetic field quanta produced by incoherent scattering (or alsoan extent of any transmitted remaining portion of the beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional electromagnetic field quanta applied) are utilized byelectromagnetic-type utilizing media comprising electrically chargedparticles comprised in the ophthalmic treatment site (8H) by processeswhich involve electromagnetic interaction so to produce the respectiveresult of non-invasive ophthalmic surgery (e.g., photocoagulation of theophthalmic treatment site when a beam of partly electromagneticallyneutralized and partly electromagnetically functional electromagneticfield quanta is applied which produces a beam of electromagneticallyfunctional electromagnetic field quanta which produces a sufficienttime-average electric flux density in the ophthalmic treatment siteafter incoherent scattering). (Note, the beam of electromagneticallyfunctional electromagnetic field quanta which is transmitted to atreatment site might adversely electromagnetically interact with anextent of the electrically charged particles surrounding a treatmentsite so to produce adverse electromagnetic effects due to thelimitations of the localization of the beam of electromagneticallyfunctional electromagnetic field quanta produced in the respectivetreatment site by incoherent scattering in such preferred embodiments ofthe present invention as the preferred embodiment herein.)

FIG. (43) is a preferred embodiment which shows the surgical arrangementof the present invention during non-invasive ophthalmic surgery of apatient by an ophthalmic surgeon. The steps applied in the preferredembodiment in FIG. (42) are, in general, applied in the preferredembodiment in FIG. (43).

In the preferred embodiment in FIG. (43), apparatus, (which is isolatedfrom mechanical vibrations) produces a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional electromagnetic field quanta which is coherently transmittedby coherent transmission media comprised by a filter, air, a surgicalcontact lens, and healthy ocular media to an ophthalmic treatment sitein an eye of a surgically prepared patient, such that adverseelectromagnetic interaction of the beam of partly electromagneticallyneutralized and partly electromagnetically functional electromagneticfield quanta with electrically charged particles comprised in thecoherent transmission media (comprising healthy ocular media) iseliminated to an extent (e.g., Rayleigh scattering and respective beambroadening, and resonance absorption and respective heating of healthyocular Media can be eliminated to an extent). Wherein, the adverseelectromagnetic effects of transmitting energy for non-invasiveophthalmic surgery are eliminated to an extent (e.g., opacification ofclear ocular media located anterior to the treatment site or also thedestruction of healthy retinal tissue surrounding the treatment site canbe eliminated to an extent).

Then, the beam of partly electromagnetically neutralized and partlyelectromagnetically functional electromagnetic field quanta isincoherently scattered to an extent by incoherently scattering mediacomprised in the treatment site so to produce a beam ofelectromagnetically functional electromagnetic field quanta (not shown)(comprising a non-zero magnitude of time-average electric flux density)in the ophthalmic treatment site (i.e., a beam of electromagneticallyfunctional electromagnetic field quanta is produced comprisingelectromagnetically functional electromagnetic field quanta produced byincoherent scattering or also comprising any remaining portion of thebeam of partly electromagnetically neutralized and partlyelectromagnetically functional electromagnetic field quanta applied).

Also, in this step, transmission media comprised in the ophthalmictreatment site transmit an extent of the electromagnetically functionalelectromagnetic field quanta produced by incoherent scattering (or alsotransmit an extent of any remaining portion of the beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional electromagnetic field quanta applied which is notincoherently scattered) to electromagnetic-type utilizing mediacomprising electrically charged particles comprised in the ophthalmictreatment site. Finally, an extent of the transmittedelectromagnetically functional electromagnetic field quanta (i.e., anextent of the transmitted electromagnetically functional electromagneticfield quanta produced by incoherent scattering or also an extent of anyremaining portion of the beam partly electromagnetically neutralized andpartly electromagnetically functional electromagnetic field quantaapplied) is utilized by way of electromagnetic interaction byelectromagnetic-type utilizing media comprising electrically chargedparticles comprised in the ophthalmic treatment site to produce therespective result of non-invasive ophthalmic surgery (e.g.,photocoagulation of the ophthalmic treatment site when a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional electromagnetic field quanta is applied which produces a beamof electromagnetically functional electromagnetic field quanta whichproduces a sufficient time-average electric flux density in theophthalmic treatment site after incoherent scattering).

FIG. (44) shows a plan side view of a preferred embodiment of thepresent invention which is applied for performing imaging in aneffective manner. In the embodiment in FIG. (44), adverseelectromagnetic interaction of wave-particle behaving entities with animaging specimen are eliminated to an extent, hence the adverseelectromagnetic effects of transmitting energy for imaging areeliminated to an extent (e.g. the destruction of an imaging specimenand/or image distortion in an imaging process can be eliminated to anextent). Steps comprised in the preferred embodiments in FIGS. (10),(11), and/or (17) or (20) can be applied, in general, in the preferredembodiment in FIG. (44) with respective modifications.

In the preferred embodiment in FIG. (44), more specifically, apparatus(2J) produces a beam of electromagnetically neutralized wave-particlebehaving entities (4J). Then, the beam of electromagneticallyneutralized wave-particle behaving entities is coherently transmitted toan extent, for example, in the form of beam (4K), by coherenttransmission media comprised in the filter (34J), the air (or vacuum,i.e., evacuated space, e.g., for an inanimate object) (42J), andcoherent transmission media (38J) comprised in the imaging specimen(44J) to any such attenuating media (46J) (drawn in a general way in theform of miniature blocks) comprised in the imaging specimen (44J);and/or to an extent, for example, in the form of beam (4L), to an imageprocessor (48J). Wherein, adverse electromagnetic interaction of thebeam of electromagnetically neutralized wave-particle behaving entitieswith electrically charged particles comprised in the coherenttransmission media comprised in the imaging specimen (44J) is eliminatedto an extent, and thus the adverse electromagnetic effects oftransmitting energy for imaging are eliminated to an extent. (Note, theuse of a beam of totally electromagnetically neutralized wave-particlebehaving atomic nuclei is not recommended for imaging because of the useof a beam of totally electromagnetically neutralized wave-particlebehaving atomic nuclei, e.g., a beam of totally electromagneticallyneutralized wave-particle behaving protons, for cold nuclear fusion inthe preferred embodiment in FIG. (30);

Herein, a filter is applied to remove unwanted electromagneticallyfunctional wave-particle behaving entities from the beam ofelectromagnetically neutralized wave-particle behaving entities appliedby way of electromagnetic interaction to prevent unwanted adverseelectromagnetic interaction of any electromagnetically functionalwave-particle behaving entities from the beam of electromagneticallyneutralized wave-particle behaving entities (4J) (produced by systematicand/or random error) by way of electromagnetic interaction withelectrically charged particles comprised in the imaging specimen (e.g.,so to decrease the radiation absorbed dose (RAD) of soft healthybiological tissue of a patient if imaging is, for example, applied formedical diagnostic imaging). Thus, an extent of the adverseelectromagnetic effects of imaging (e.g., the destruction of the imagingspecimen and/or image distortion) can be eliminated to an extent (e.g.,the destruction of soft healthy biological tissue in a patient anddistortion of the image of the respective patient can be eliminated toan extent if imaging is applied for medical diagnostic imaging).

If any such attenuating media (46J) in the respective imaging specimenincoherently deflect in the forward direction (e.g., incoherentlyscatter in the forward direction) an extent of the beam ofelectromagnetically neutralized wave-particle behaving entities (4J) soto eliminate an extent of the destructive interference of waves andrespective cancellation of associated time-varying electric and magneticfields from beam (4J) so to produce electromagnetically functionalwave-particle behaving entities (comprising a non-zero magnitude oftime-average electric flux density), then, conditionally, an extent ofsuch electromagnetically functional wave-particle behaving entitiesproduced by incoherently deflecting attenuating media, or also an extentof any remaining portion of the beam of electromagnetically neutralizedwave-particle behaving entities applied which is coherently transmittedby coherent transmission media (38J) comprised in the imaging specimenand air (or vacuum, i.e., evacuated space, e.g., for an inanimateobject) (or coherently deflected in then forward direction by anycoherently deflecting attenuating media) would be transmitted to theimage processor (48J). In this case, attenuating media (46J) cancomprise: A) potential-energy-type attenuating media which comprise aregularly ordered distribution of particles or an irregularly ordereddistribution of particles (e.g., media equivalent topotential-energy-type incoherently scattering media as described in thepreferred embodiment in FIG. (13)) which each comprise: a) potentialenergy which changes significantly relative to the potential energycomprised by respective surroundings and the total energy comprised bywave-particle behaving entities respectively deflected from beam (4J);and b) a size and spacing which are smaller than, comparable to, orsignificantly larger than, the wavelength of the waves comprised bywave-particle behaving entities respectively deflected from beam (4J).Wherein, potential-energy-type attenuating processes involve a quantummechanical functional relation between the potential energy comprised bythe potential-energy-type attenuating media (46J) and the total energycomprised by respectively deflected wave-particle behaving entities;and/or, B) attenuating media (46J) can comprise electromagnetic-typeattenuating media comprising: a) a regularly order distribution ofelectrically charged particles or an irregularly ordered distribution ofelectrically charged particles (e.g., media equivalent toelectromagnetic-type incoherently scattering media as described in thepreferred embodiment in FIG. (14)) comprising electrically chargedparticles (e.g., atoms and molecules) which each comprise spacing whichis smaller than, comparable to, or significantly larger than thewavelength of the waves comprised by the respectively deflectedwave-particle behaving entities; and/or b) electromagneticallyabsorptive media (e.g., resonance absorptive media). Wherein,electromagnetic-type attenuation processes involve electromagneticinteraction. (Note, if a beam of totally electromagnetically neutralizedwave-particle behaving entities is applied in the preferred embodimentin FIG. (44), then, electromagnetic-type attenuation (e.g.,electromagnetic-type incoherent scattering) of electromagneticallyfunctional wave-particle behaving entities by attenuating media wouldoccur dependent upon the onset of the production of theelectromagnetically functional wave-particle behaving entities bypotential-energy-type attenuation (i.e., potential-energy-typeincoherent scattering). However, if a beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities is applied in the preferred embodiment in FIG. (44),then electromagnetic-type attenuation of electromagnetically functionalwave-particle behaving entities would occur independent of the onset ofthe production of the electromagnetically functional wave-particlebehaving entities by potential-energy-type attenuation, since a beam ofpartly electromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities already compriseswave-particle behaving entities which are electromagnetically functionalto an extent, i.e., partly electromagnetically neutralized and partlyelectromagnetically functional.)

Some methods of utilizing wave-particle behaving entities transmitted tothe image processor (48J) to form an image are possible:

In a first method, any coherently transmitted electromagneticallyneutralized wave-particle behaving entities can be utilized by apparatuscomprising momentum-type utilizing apparatus (e.g., an array of MEMSpressure sensors) (as described, in general, in the preferred embodimentin FIG. (10)) to form an image;

In a second method, any electromagnetically functional wave-particlebehaving entities (comprising a non-zero magnitude of time-averageelectric flux density) produced by attenuating media (46J) (and/or anyremaining portion of a beam of partly electromagnetically neutralizedand partly electromagnetically functional wave-particle behavingentities if a beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities isapplied) which is transmitted to the image processor (48J) can beutilized by way of electromagnetic interaction by electromagnetic-typeutilizing apparatus comprising electrically charged particles comprisedin the image processor (48J) (as described, in general, in the preferredembodiment in FIG. (11)) to form an image;

In a third method, the image processor (48J) can comprise apparatuscomprising coherent transmission media and electromagneticallyfunctional media (e.g., electromagnetically photo-reactive mediacomprising electrically charged particles; or an electrostatic,electromagnetic, or magnetic deflecting apparatus as the circumstancesrequire (which includes apparatus for detecting respectively deflectedelectromagnetically functional wave-particle behaving entities by way ofelectromagnetic interaction), i.e., apparatus similar to a passive-typefiltering apparatus as described in the preferred embodiment in FIG.(23) except, in this case, such apparatus would be used to produce animage in an imaging process). Wherein, any electromagneticallyfunctional wave-particle behaving entities (comprising a non-zeromagnitude of time-average electric flux density) produced by attenuatingmedia (46J), or also any remaining portion of a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities, if a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities is applied, which istransmitted to the image processor (48J) would be utilized by suchapparatus to form an image.

In addition, any totally electromagnetically neutralized wave-particlebehaving entities which are coherently transmitted to such anelectromagnetic-type utilizing and coherently transmitting apparatuscomprised in the image processor (48J) can be coherently transmitted bysuch apparatus to apparatus located posteriorly which could, asexamples: a) utilize the coherently transmitted totallyelectromagnetically neutralized wave-particle behaving entities by amomentum utilizing process which applies a momentum-type utilizingapparatus (e.g., an array of MEMS pressure sensors) (as described, ingeneral, in the preferred embodiment in FIG. (10)); or b) incoherentlyscatter the totally electromagnetically neutralized wave-particlebehaving entities so to produce electromagnetically functionalwave-particle behaving entities (with a corresponding non-zero magnitudeof time-average electric flux density) in the image processor (48J).Wherein, transmission media in the image processor (48J) would transmitsuch electromagnetically functional wave-particle behaving entities toelectromagnetic-type utilizing apparatus comprising electrically chargedparticles comprised in the image processor (48J), which would thenutilize transmitted electromagnetically functional wave-particlebehaving entities by way of electromagnetic interaction (as described,in general, in the preferred embodiment in FIG. (17) or (20)) to form animage. Thus, the third method of forming an image in the preferredembodiment in FIG. (44) can produce two separate images of the imagingspecimen (44J) (i.e., can produce one image from electromagneticallyfunctional wave-particle behaving entities produced by attenuation, andcan produce another image from electromagnetically neutralizedwave-particle behaving entities coherently transmitted by the imagingspecimen. (Note, here the apparatus which utilizes electromagneticallyfunctional wave-particle behaving entities from beam (4L), and which isalso coherently transmitting, also eliminates the sameelectromagnetically functional wave-particle behaving entities from beam(4L) so to produce a beam of totally electromagnetically neutralizedwave-particle behaving entities, which is transmitted to the utilizingapparatus located posteriorly, thus acting like a passive-type filteringapparatus as described in the preferred embodiment in FIG. (23).); and,

In a fourth method, the last utilizing apparatus aforedescribed in thethird method (i.e., apparatus comprising incoherent scattering,transmitting, and utilizing apparatus) can be applied exclusively by theimage processor (48J) to form an image in an embodiment of the presentinvention for imaging which applies a beam of totallyelectromagnetically neutralized wave-particle behaving entities.Wherein, any electromagnetically functional wave-particle behavingentities (comprising a non-zero magnitude of time-average electric fluxdensity) produced by attenuating media (46J), or also any remainingportion of a beam of electromagnetically neutralized wave-particlebehaving entities if a beam of partly electromagnetically neutralizedand partly electromagnetically functional wave-particle behavingentities is applied, which are transmitted to such a utilizing apparatuscomprised in the image processor (48J) can be incoherently scattered bysuch apparatus in the image processor (48J) so to effectively produceelectromagnetically functional wave-particle behaving entities (with acorresponding a non-zero magnitude of time-average electric fluxdensity) in the image processor (48J). Also, transmission media in suchapparatus in the image processor (48J) would transmit suchelectromagnetically functional wave-particle behaving entities toelectromagnetic-type utilizing apparatus comprising electrically chargedparticles comprised in the image processor (48J) which would utilize thetransmitted electromagnetically functional wave-particle behavingentities by way of electromagnetic interaction to form an image asdescribed for such apparatus in the third method of forming an imagehereinbefore. (Note, if any such attenuating media (46J) in therespective imaging specimen incoherently scatter an extent of the beamof electromagnetically neutralized wave-particle behaving entities (4J)so to produce electromagnetically functional wave-particle behavingentities (comprising a non-zero magnitude of time-average electric fluxdensity) in the imaging specimen, or if a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities is applied in the preferredembodiment in FIG. (44), then after transmission of suchelectromagnetically functional wave-particle behaving entities toelectrically charged particles comprised in the imaging specimen, suchelectrically charged particles can adversely electromagneticallyinteract with any such electromagnetically functional wave-particlebehaving entities and produce corresponding adverse electromagneticeffects (e.g., adversely destroy the imaging specimen to an extentand/or create image distortion to an extent. Also, note that an imagingspecimen may be absent of any such attenuating media, in which case, acorresponding image would be formed indicating such a condition.)

FIG. (45) shows a plan side view of another preferred embodiment of thepresent invention which is applied for performing imaging in aneffective manner. Steps comprised in the preferred embodiment in FIGS.(44) and (19) can be applied in the preferred embodiment in FIG. (45)with some respective modifications.

In the preferred embodiment in FIG. (45), apparatus (2M) produces a beamof electromagnetically neutralized wave-particle behaving entities (4M)which is coherently transmitted to an extent, for example, in the formof beam (4N), by coherent transmission media comprised in the filter(34M), the air (or vacuum, i.e., evacuated space, e.g., for an inanimateobject) (42M), and coherent transmission media (38M) comprised in theimaging specimen (44M) to any such attenuating media (46M) (drawn in ageneral way in the form of miniature blocks) comprised in the imagingspecimen (44M), and/or coherently transmitted to an extent, for example,in beam (4P), to the shielding apparatus (50), such that adverseelectromagnetic interaction of the beam of electromagneticallyneutralized wave-particle behaving entities with electrically chargedparticles comprised in the coherent transmission media (in the imagingspecimen) is eliminated to an extent. Wherein, the adverseelectromagnetic effects of transmitting energy for imaging areeliminated to an extent (e.g., the destruction of an imaging specimenand/or image distortion in the imaging process is eliminated to anextent).

If any such attenuating media (46M) in the respective imaging specimenincoherently backscatter an extent of the beam of electromagneticallyneutralized wave-particle behaving entities (4M), then, conditionally,an extent of any electromagnetically functional wave-particle behavingentities produced by incoherent backscattering, or also an extent of anybackwardly and laterally deflected portion of the beam ofelectromagnetically neutralized wave-particle behaving entities applied,for example, in the form of beam (4R), would be transmitted, orcoherently transmitted, respectively, by transmission media, or coherenttransmission media, respectively, comprised in the imaging specimen andthe air (or vacuum, i.e., evacuated space, e.g., for an inanimateobject) (42M) to the image processor (48M). Furthermore, an extent ofany electromagnetically neutralized wave-particle behaving entitieswhich are coherently transmitted in the forward direction; and an extentof any electromagnetically functional wave-particle behaving entitiesproduced by attenuation (e.g., incoherent scattering) which istransmitted in the forward direction, can all be transmitted in the formof beam (4P) to the shielding apparatus (50).

Herein, attenuating media (46M) and the filter (34M) comprise parametersas described in the preferred embodiment in FIG. (44); an image isformed in the image processor (48M) by methods equivalent to the methodsfor forming an image which are described in the preferred embodiment inFIG. (44); and the beam of wave-particle behaving entities (comprisingany coherently transmitted electromagnetically neutralized wave-particlebehaving entities and/or any transmitted electromagnetically functionalwave-particle behaving entities produced by attenuation, including anycoherently transmitted remaining portion of a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities which was not incoherentlyscattered if a beam of partly electromagnetically neutralized and partlyelectromagnetically functional wave-particle behaving entities isapplied, is discarded by the shielding apparatus (50)). Here, theshielding apparatus (50) comprises electromagnetic-type incoherentlyscattering and transmitting media, potential-energy-type incoherentlyscattering and transmitting media, and electromagnetically absorptivemedia. Wherein, the shielding apparatus (50) would absorb anyelectromagnetically functional wave-particle behaving entitiestransmitted to the shielding apparatus, or incoherently scatterselectromagnetically neutralized wave-particle behaving entitiestransmitted to the shielding apparatus, and transmits and then absorbsthe particular type of electromagnetically functional wave-particlebehaving entities which result in the respective shielding apparatus(50). (Note, that an imaging specimen may be absent of any suchattenuating media, in which case, a corresponding image would be formedindicating such a condition. Also, note that the use of a beam oftotally electromagnetically neutralized atomic nuclei is not recommendedfor imaging because of the use of a beam of totally electromagneticallyneutralized wave-particle behaving atomic nuclei, e.g., a beam oftotally electromagnetically neutralized wave-particle behaving protons,for cold nuclear fusion in the preferred embodiment in FIG. (30).)

Another preferred embodiment of the present invention for imaging couldcombine aspects of the preferred embodiments applied for imaging inFIGS. (44) and (45). Wherein, such a preferred embodiment for imagingwould apply a method which would produce an image from energytransmitted in both the forward and backward directions.

FIG. (46) shows a longitudinally sectioned view of a preferredembodiment of the present invention which is applied for efficientlytransmitting power. The steps applied in preferred embodiments, asexamples, in FIG. (10), (11), (17), or (20) can be applied in thepreferred embodiment in FIG. (46) with some respective modifications.

In the preferred embodiment in FIG. (46), more specifically, apparatus(2S) produces a beam of electromagnetically neutralized wave-particlebehaving entities (4S) which is coherently transmitted by coherenttransmission apparatus comprising the air (36S) and the tubing (38S) topower utilizing apparatus (8S), such that adverse electromagneticinteraction of the beam of electromagnetically neutralized wave-particlebehaving entities with electrically charged particles comprised in thecoherently transmitting tubing is eliminated to an extent. Wherein, theadverse electromagnetic effects of transmitting energy for power areeliminated to an extent (e.g., power attenuation is eliminated to anextent).

In this case, coherently transmitting tubing comprises tubing wallswhich produce a potential energy barrier which changes significantlyrelative to the potential energy comprised by its respectivesurroundings (e.g., air inside and outside the tubing) and the totalenergy comprised by the coherently transmitted electromagneticallyneutralized wave-particle behaving entities in beam (4S); and comprisesparticles which comprise electrically charged particles on the innersurface of the tubing which comprise a size and spacing which are eachsignificantly smaller than the wavelength of the waves comprised in thebeam of electromagnetically neutralized wave-particle behaving entities(4S). Wherein, coherent transmission processes involve a quantummechanical functional relation between the potential energy comprised bythe tubing (38S) and the total energy comprised by coherentlytransmitted electromagnetically neutralized wave-particle behavingentities in beam (4S); or also coherent transmission processes involveelectromagnetic interaction if a beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities is applied.

Then, the power utilizing apparatus (8S) utilizes transmittedwave-particle behaving entities by an appropriate process for powerutilization (e.g., a) a process which includes utilization of momentumby a momentum-type utilizing apparatus (as described generally in thepreferred embodiment in FIG. (10)); or b) a process in whichelectromagnetic-type utilizing apparatus, comprising electricallycharged particles, utilizes partly electromagnetically neutralized andpartly electromagnetically functional wave-particle behaving entities byway of electromagnetic interaction when a beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities is applied (as describedgenerally in the preferred embodiment in FIG. (11)); or c) a processwhich includes the incoherent scattering of coherently transmittedelectromagnetically neutralized wave-particle behaving entities byincoherently scattering media so to produce a beam ofelectromagnetically functional wave-particle behaving entities (whichcomprises a non-zero magnitude of time-average electric flux density)(i.e., a beam of electromagnetically functional wave-particle behavingentities comprising electromagnetically functional wave-particlebehaving entities produced by incoherent scattering or also comprisingany remaining portion of a beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities which is not incoherently scattered if a beam ofpartly electromagnetically neutralized and partly electromagneticallyfunctional wave-particle behaving entities is applied) (as describedgenerally in the preferred embodiments in FIGS. (17) and (20)); which istransmitted by transmission media (comprised in the power utilizingapparatus) to an electromagnetic-type utilizing apparatus comprisingelectrically charged particles; which then utilizes the transmittedelectromagnetically functional wave-particle behaving entities forpower. (Note, the use of a beam of totally electromagneticallyneutralized wave-particle behaving atomic nuclei for transmitting poweris not recommended as specifically relates to the preferred embodimentdescribed herein because of the use of a beam of totallyelectromagnetically neutralized wave-particle behaving atomic nuclei,e.g., a beam of totally electromagnetically neutralized wave-particlebehaving protons, for cold nuclear fusion in the preferred embodiment inFIG. (30)).

FIG. (47) includes a longitudinal view of the tubing of anotherpreferred embodiment of the present invention which is applied forefficiently transmitting power. The steps applied in the preferredembodiment in FIG. (46) are basically applicable in the preferredembodiment in FIG. (47) except, as a modification, two tube branchesmerge into a single section of tubing.

Wherein, in the preferred embodiment in FIG. (47), two apparatus eachproduce a beam of electromagnetically neutralized wave-particle behavingentities which are each coherently transmitted by a respective tubingsection, and then are combined by a merged tubing section into a singlebeam of electromagnetically neutralized wave-particle behaving entitieswhich is transmitted in a coherent manner to a power utilizing apparatus(i.e., the merged tubing acts as a coupler).

Here, the beams of electromagnetically neutralized wave-particlebehaving entities are each coherently transmitted by a respectivesection of tubing, such that adverse electromagnetic interaction of thebeams of electromagnetically neutralized wave-particle behaving entitieswith electrically charged particles comprised in a respective tubingsection is eliminated to an extent. Wherein, the adverse electromagneticeffects of transmitting energy for power are eliminated to an extent(e.g., power attenuation is eliminated to an extent). Then, eachutilizing apparatus utilizes a respective coherently transmitted beam ofelectromagnetically neutralized wave-particle behaving entities by aprocess for power utilization (as described, in general, in thepreferred embodiment in FIG. (46)).

FIG. (48) includes a longitudinal view of the tubing of anotherpreferred embodiment of the present invention which is applied forefficiently transmitting power. The steps applied in the preferredembodiment in FIG. (48) are basically applicable in the preferredembodiment in FIG. (48) except, as a modification, the tube branchesinto two tube branches.

Wherein, in the preferred embodiment in FIG. (46), apparatus produces abeam of electromagnetically neutralized wave-particle behaving entitieswhich is coherently transmitted by tubing to a branching in the tubing,and then is divided by the branched tubing into two respective beamfractions of electromagnetically neutralized wave-particle behavingentities (i.e., the branched tubing acts as a splitter). Then, the twotube branches each transmit a respective beam fraction ofelectromagnetically neutralized wave-particle behaving entities in acoherent manner to a respective power utilizing apparatus.

Here, the beam of electromagnetically neutralized wave-particle behavingentities and each respective beam fraction of electromagneticallyneutralized wave-particle behaving entities is coherent transmitted by arespective section of tubing, such that adverse electromagneticinteraction of the beam and beam fractions of electromagneticallyneutralized wave-particle behaving entities with electrically chargedparticles comprised in a respective tubing section is eliminated to anextent. Wherein, the adverse electromagnetic effects of transmittingenergy for power are eliminated to an extent (e.g., power attenuation iseliminated to an extent). Then the coherently transmitted beam fractionsof electromagnetically neutralized wave-particle behaving entities areeach utilized by respective utilizing apparatus by a process for powerutilization (as described, in general, in the preferred embodiment inFIG. (46)).

FIG. (49) includes a longitudinal view of the tubing of anotherpreferred embodiment of the present invention which is applied forefficiently transmitting power. The steps applied in the preferredembodiments in FIGS. (47) and (48) are basically applicable in thepreferred embodiment in FIG. (49) except, as a modification, two tubebranches merge into a single section of tubing (i.e., the merged tubingacts as a coupler), and then the single section of tube branches intotwo tube branches (i.e., the branched tubing acts as a splitter).

Other embodiments for efficiently transmitting power can basically applythe steps applied in the preferred embodiment in FIG. (46) with theexception that optical fiber is applied for efficiently transmittingpower instead of tubing. Wherein, in such a preferred embodiment,apparatus produces a beam of electromagnetically neutralizedwave-particle behaving entities which is coherently transmitted by anoptical fiber to a power utilizing apparatus, such that adverseelectromagnetic interaction of the beam of electromagneticallyneutralized wave-particle behaving entities with electrically chargedparticles comprised in the optical fiber is eliminated to an extent.Wherein, the adverse electromagnetic effects of transmitting energy forpower (e.g., power attenuation) are eliminated to an extent.

In this case, the coherently transmitting optical fiber comprisesoptical fiber core which comprises potential energy which changessignificantly relative to the potential energy comprised by therespectively comprised cladding and relative to the total energycomprised by the coherently transmitted electromagnetically neutralizedwave-particle behaving entities so to produce a significant potentialenergy barrier (which effectively produces total internal reflection);and the optical fiber core comprises particles, which compriseelectrically charged particles, and comprise: a) potential energy whichchanges insignificantly relative to the potential energy comprised byits respective surroundings and the total energy comprised by thewave-particle behaving entities in the coherently transmitted beam ofelectromagnetically neutralized wave-particle behaving entities; and b)a size and spacing which are each significantly smaller than thewavelength of the waves comprised in the beam of electromagneticallyneutralized wave-particle behaving entities. Wherein, coherenttransmission processes involve a quantum mechanical functional relationbetween the potential energy comprised by the optical fiber and thetotal energy comprised by coherently transmitted electromagneticallyneutralized wave-particle behaving entities in the coherentlytransmitted beam; or also coherent transmission processes involveelectromagnetic interaction if a beam of partly electromagneticallyneutralized and partly electromagnetically functional wave-particlebehaving entities is applied. Then, utilizing apparatus utilizes thecoherently transmitted beam of electromagnetically neutralizedwave-particle behaving entities by a process for power utilization (asdescribed, in general, in the preferred embodiment in FIG. (46)).

FIG. (50) shows a preferred embodiment of the present invention which isapplied for efficient wireline-type communications. The steps applied inthe preferred embodiments for power transmission in FIGS. (46), (47),(48), (49), and the optical fiber preferred embodiment previouslydescribed are basically applicable to the preferred embodiment in FIG.(50) for wireline-type communications with some respectivemodifications.

In the preferred embodiment in FIG. (50), more specifically, apparatuscomprising a transmitter apparatus produces a beam ofelectromagnetically neutralized electromagnetic field quanta. Then, thebeam of electromagnetically neutralized electromagnetic field quanta iscoherently transmitted and modulated by a modulator which comprisescoherent transmission media, and which changes its respective potentialenergy in order to modulate (e.g., a pulse modulator comprising, forexample, an acousto-optic modulator) so to produce a pulse modulatedbeam of electromagnetically neutralized electromagnetic field quantawhich encodes signals (e.g., a pulse modulated beam ofelectromagnetically neutralized electromagnetic field quanta, whichencodes data, as shown in the beam of electromagnetically neutralizedwave-particle behaving entities in FIG. (5) or (9)).

Then, the pulse modulated beam of electromagnetically neutralizedelectromagnetic field quanta is coherently transmitted by coherenttransmitting media comprised by the tubing apparatus to the receivingapparatus, such that adverse electromagnetic interaction of the beam ofelectromagnetically neutralized electromagnetic field quanta withelectrically charged particles comprised in the coherently transmittingtubing is eliminated to an extent. Wherein, the adverse electromagneticeffects of transmitting energy for communications are eliminated to anextent (e.g., signal attenuation is eliminated to an extent so toincrease the distance a signal can travel at various wavelengths withoutbeing repeated, and thus also increase the bandwidth available forwireline-type communications).

Then, the coherently transmitted beam of electromagnetically neutralizedelectromagnetic field quanta is utilized by an appropriate process forcommunications reception (e.g., a receiving process which includesutilizing momentum for communications reception with a momentum-typeutilizing apparatus comprising, for example, a pressure transducer (asdescribed generally in the preferred embodiment in FIG. (10)); or b) areceiving process in which electromagnetic-type utilizing apparatus,comprising electrically charged particles, utilizes partlyelectromagnetically neutralized and partly electromagneticallyfunctional electromagnetic field quanta by way of electromagneticinteraction when a beam of partly electromagnetically neutralized andpartly electromagnetically functional electromagnetic field quanta isapplied for communications (as described generally in the preferredembodiment in FIG. (11)); or c) a receiving process which includes theincoherent scattering of coherently transmitted electromagneticallyneutralized electromagnetic field quanta by incoherently scatteringmedia so to produce a beam of electromagnetically functionalelectromagnetic field quanta (which comprises a non-zero magnitude oftime-average electric flux density) (i.e., a beam of electromagneticallyfunctional wave-particle behaving entities comprisingelectromagnetically functional electromagnetic field quanta produced byincoherent scattering or also comprising any remaining portion of a beamof partly electromagnetically neutralized and partly electromagneticallyfunctional electromagnetic field quanta which is not incoherentlyscattered if a beam of partly electromagnetically neutralized and partlyelectromagnetically functional electromagnetic field quanta isapplied)); which is also transmitted by transmission media (comprised inthe receiving apparatus) to an electromagnetic-type utilizing apparatuscomprising electrically charged particles comprised in the receivingapparatus; which then utilizes the transmitted electromagneticallyfunctional electromagnetic field quanta by way of electromagneticinteraction for communications reception (as described generally in thepreferred embodiment in FIG. (17) or (20)).

FIG. (51) shows a preferred embodiment of the present invention which isapplied for efficient wireless-type communications. The steps applied inthe preferred embodiment in FIG. (50) are basically applicable in thepreferred embodiment in FIG. (51) except that the preferred embodimentin FIG. (51) applies air for coherent transmission media instead oftubing.

FIG. (52) shows another preferred embodiment of the present inventionwhich is applied for efficient wireless-type communications. The stepsapplied in the preferred embodiment in FIG. (12) are basicallyapplicable in the preferred embodiment in FIG. (52) with somemodifications.

In the preferred embodiment in FIG. (52) a transmitter apparatusproduces a beam of partly electromagnetically neutralized and partlyelectromagnetically functional electromagnetic field quanta whichcomprises at least two linearly polarized coherent beams ofelectromagnetic field quanta which each comprise a plane of polarizationwith a slightly different angle of rotation, or also are superimposedpartly out of phase. Then, the beam of partly electromagneticallyneutralized and partly electromagnetically functional electromagneticfield quanta is coherently transmitted by coherent transmission mediacomprising a modulator (e.g., an acousto-optic modulator which comprisescoherent transmission media and modulates by changing its respectivepotential energy) so as to produce a modulated beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional electromagnetic field quanta which encodes data, andsubsequently coherently transmitted by coherent transmission mediacomprised by air to a receiving apparatus comprising a polarizer (orpolarizers) and an electromagnetic-type detecting apparatus (e.g., anantenna or a photodetector according to the wavelength of the linearlypolarized beam electromagnetically functional electromagnetic fieldquanta applied).

Wherein, during coherent transmission, adverse electromagneticinteraction of the modulated beam of partly electromagneticallyneutralized and partly electromagnetically functional electromagneticfield quanta with electrically charged particles comprised in thecoherently transmitting air is eliminated to an extent. Wherein, theadverse electromagnetic effects of transmitting energy for wireless-typecommunications are eliminated to an extent (e.g., signal attenuation iseliminated to an extent so to increase the distance a signal can travelat various wavelengths without being repeated, and thus also increasethe bandwidth available for wireless-type communications).

Then, for example, the linearly polarized coherent beam portions ofelectromagnetic field quanta comprised in the coherently transmittedbeam of partly electromagnetically neutralized and partlyelectromagnetically functional electromagnetic field quanta can beseparated into respective individual linearly polarized coherent beamportions of electromagnetic field quanta along a respective Brewster'sangle by the polarizing apparatus, such that destructive interference ofwaves and respective cancellation of associated time-varying electricand magnetic fields in the coherently transmitted beam of partlyelectromagnetically neutralized and partly electromagneticallyfunctional electromagnetic field quanta are respectively eliminated.Wherein, in effect, a plurality of individual linearly polarized beamsof electromagnetically functional electromagnetic field quanta areproduced. In any such case, polarization involves electromagneticinteraction. Also, step 3) comprises the transmission of each of thelinearly polarized beams of electromagnetically functionalelectromagnetic field quanta by transmission apparatus comprised in therespective polarizer (or also comprised in the electromagnetic-typedetecting apparatus) comprised in the receiving apparatus to respectiveelectromagnetic-type detecting apparatus comprising electrically chargedparticles; and, then,

Step 4) the utilization of each of the transmitted linearly polarizedbeams of electromagnetically functional electromagnetic field quanta bya respective electromagnetic-type detecting apparatus comprised in therespective receiving apparatus by way of electromagnetic interaction forwireless-type communications reception.

FIG. (53) shows another preferred embodiment of the present inventionwhich is applied for efficient wireline-type communications. The stepsapplied in the preferred embodiment in FIG. (50) are applicable in thepreferred embodiment in FIG. (53) except that the method ofcommunications in the preferred embodiment in FIG. (53) appliesmultiplexing and demultiplexing (i.e., here, wave division multiplexingand wave division demultiplexing).

Wherein, in the preferred embodiment in FIG. (53), apparatus comprisinga plurality of transmitter apparatus produces a plurality of beams ofelectromagnetically neutralized electromagnetic field quanta which eachcomprise a different linewidth. Then, the beams of electromagneticallyneutralized electromagnetic field quanta of different linewidths arecoherently transmitted and modulated by respective modulators (whicheach modulates by changing its respective potential energy, e.g., acoherently transmissive acousto-optic modulator) so to producerespective pulse modulated beams of electromagnetically neutralizedelectromagnetic field quanta which each comprise a respectivelydifferent linewidth and encodes signals. Then, the pulse modulated beamsof electromagnetically neutralized electromagnetic field quanta arecoherently transmitted to, and multiplexed by, a multiplexer so toproduce a multiplexed beam of electromagnetically neutralizedelectromagnetic field quanta.

Subsequently, the multiplexed beam of electromagnetically neutralizedelectromagnetic field quanta is coherently transmitted by coherenttransmission media comprising tubing apparatus to a demultiplexer, suchthat adverse electromagnetic interaction of the multiplexed beam ofelectromagnetically neutralized electromagnetic field quanta withelectrically charged particles comprised in the coherently transmittingtubing is eliminated to an extent. Wherein, the adverse electromagneticeffects of transmitting energy for wireline-type communications areeliminated to an extent (e.g., signal attenuation is eliminated to anextent so to increase the distance a signal can travel at variouswavelengths without being repeated, and thus also increase the bandwidthavailable for wireline-type communications).

Then, the demultiplexer demultiplexes the multiplexed beam ofelectromagnetically neutralized electromagnetic field quanta intoseparate beams of electromagnetically neutralized electromagnetic fieldquanta of respective linewidths, which then are coherently transmittedto respective apparatus comprised in a receiving apparatus whichutilizes the respective coherently transmitted beam ofelectromagnetically neutralized electromagnetic field quanta by anappropriate process for communications reception (e.g., one of thereceiving processes described in the preferred embodiment in FIG. (50)).

FIG. (53A) shows another preferred embodiment which applies multiplexingand demultiplexing for efficient wireline-type communications. FIG.(53A) is a more detailed example of a preferred embodiment of thepresent invention in FIG. (53). The steps applied in the preferredembodiment in FIG. (53) are applicable in the preferred embodiment inFIG. (53A) except, more specifically, the preferred embodiment in FIG.(53A) applies a prism as a multiplexer and a prism as a demultiplexer.

FIG. (53B) shows another preferred embodiment which applies multiplexingand demultiplexing for efficient wireline-type communications. FIG.(53B) is also a more detailed example of a preferred embodiment of thepresent invention in FIG. (53). The steps applied in the preferredembodiment in FIG. (53) are applicable in the preferred embodiment inFIG. (53B) except, more specifically, the preferred embodiment in FIG.(53B) applies a reflective diffraction grating as a multiplexer and areflective diffraction grating as a demultiplexer.

FIG. (54) shows another preferred embodiment of the present inventionwhich is applied for efficient wireless-type communications. The stepsapplied in the preferred embodiment in FIG. (53) are basicallyapplicable in the preferred embodiment in FIG. (54) except that thepreferred embodiment in FIG. (54) applies air for coherent transmissionmedia instead of tubing.

FIG. (55) shows another preferred embodiment of the present inventionwhich is applied for efficient wireless-type communications. The stepsapplied in the preferred embodiment in FIG. (52) are applicable in thepreferred embodiment in FIG. (55) except that the method ofcommunications in the preferred embodiment in FIG. (55) appliesmultiplexing and demultiplexing (i.e., here, wave division multiplexingand wave division demultiplexing).

Wherein, in the preferred embodiment in FIG. (55), apparatus comprisinga plurality of transmitter apparatus produces a plurality of beams ofpartly electromagnetically neutralized and partly electromagneticallyfunctional electromagnetic field quanta which each comprise a differentlinewidth and at least two linearly polarized coherent beams ofelectromagnetic field quanta which each have a plane of polarizationwith a slightly different angle of rotation, or also are superimposedpartly out of phase. Then, the beams of partly electromagneticallyneutralized and partly electromagnetically functional electromagneticfield quanta of different linewidths are each coherently transmitted andmodulated by a respective modulator (e.g., acousto-optic modulator whichcomprises coherent transmission media and changes its respectivepotential energy in order to modulate) so to produce respective pulsemodulated beams of partly electromagnetically neutralized and partlyelectromagnetically functional electromagnetic field quanta of differentlinewidths which each encode signals. Then, the pulse modulated beams ofpartly electromagnetically neutralized and partly electromagneticallyfunctional electromagnetic field quanta of different linewidths arecoherently transmitted by coherent transmission media comprised by airto, and multiplexed by, a multiplexer so to produce a multiplexed beamof electromagnetically neutralized electromagnetic field quanta.

Subsequently, the multiplexed beam of partly electromagneticallyneutralized and partly electromagnetically functional electromagneticfield quanta is coherently transmitted by coherent transmission mediacomprised by air to a demultiplexer, such that adverse electromagneticinteraction of the multiplexed beam of partly electromagneticallyneutralized and partly electromagnetically functional electromagneticfield quanta with electrically charged particles comprised in thecoherently transmitting air is eliminated to an extent. Wherein, theadverse electromagnetic effects of transmitting energy for wireless-typecommunications are eliminated to an extent (e.g., signal attenuation iseliminated to an extent so to increase the distance a signal can travelat various wavelengths without being repeated, and thus also increasethe bandwidth available for wireline-type communications).

Then, the demultiplexer demultiplexes the multiplexed beam ofelectromagnetically neutralized electromagnetic field quanta intoseparate beams of partly electromagnetically neutralized and partlyelectromagnetically functional electromagnetic field quanta ofrespective linewidths, which then are each coherently transmitted to arespective polarizer comprised in a respective receiving apparatus,which then separates out a respective linearly polarized coherent beamportion of electromagnetic field quanta comprised in the respectivecoherently transmitted beam of partly electromagnetically neutralizedand partly electromagnetically functional electromagnetic field quanta,such that destructive interference of waves and respective cancellationof associated time-varying electric and magnetic fields comprised in therespective coherently transmitted beam of partly electromagneticallyneutralized and partly electromagnetically functional electromagneticfield quanta are eliminated. Wherein, in effect, a plurality ofindividual linearly polarized beams of electromagnetically functionalelectromagnetic field quanta are produced, which then are eachtransmitted by air to a respective electromagnetic-type detectingapparatus (e.g., an antenna or a photodetector according to thewavelength of the linearly polarized beam electromagnetically functionalelectromagnetic field quanta applied), which is comprised in arespective receiving apparatus, which then each utilize the respectivelytransmitted linearly polarized beam of electromagnetically functionalelectromagnetic field quanta by way of electromagnetic interaction forwireless-type reception).

FIG. (56) shows a preferred embodiment of the present invention which isapplied for efficient energy storage. In this case, the preferredembodiment in FIG. (56) eliminates an extent of the adverseelectromagnetic interaction of a beam of electromagnetically neutralizedwave-particle behaving entities with electrically charged particlescomprised in an energy storage container, hence eliminating an extent ofthe adverse electromagnetic effects of storing energy (e.g., eliminatingan extent of the inefficiency of energy storage).

The steps applied in the preferred embodiments in FIG. (2) or (6) areapplicable, in general, in the preferred embodiment in FIG. (56).However, more specifically, the preferred embodiment in FIG. (56)comprises the following method:

Apparatus, which comprises Michelson interferometric apparatus,comprises a laser which produces a laser beam. The laser beam is divided(i.e., partly transmitted and partly reflected) by the partiallymirrored second surface of a plane beam splitter (i.e., a partlytransmitting and partly reflecting mirror) so to produce a firsttransmitted laser beam fraction, and so also to produce a firstreflected laser beam fraction. Here, the beam splitter is comprised byone side of an enclosed, sealed, storage container, which is atriangularly shaped pentahedron (five sided polyhedron) which alsocomprises a second side, a third side, top and bottom sides, andcontains a vacuum (evacuated space).

Then, the first transmitted laser beam fraction is coherentlytransmitted by the vacuum to the totally reflecting plane mirrored firstsurface comprised by the second side of the storage container; and thefirst reflected laser beam fraction is transmitted by the air (orvacuum) to a totally reflecting plane mirrored first surface comprisedby a mirror which is separate from the storage container. Then, thetotally reflecting mirror, which is comprised by the second side of thestorage container, totally reflects the first transmitted laser beamfraction in a coherent manner so that the first transmitted laser beamfraction is then coherently transmitted by the vacuum back to the beamsplitter, which then divides the first transmitted laser beam fractionso to produce a second transmitted laser beam fraction which istransmitted back towards the laser output apparatus; and so to produce asecond reflected laser beam fraction which is reflected in a coherentmanner towards the plane mirrored first surface comprised by, forexample, a microelectromechanical mirror which is attached to the thirdside of the storage container. Also, the separate totally reflectingmirror totally reflects the first reflected laser beam fraction in acoherent manner so that the first reflected laser beam fraction is thencoherently transmitted by the air (or vacuum) back to the beam splitterwhich then divides the first reflected laser beam fraction so to producea third transmitted laser beam fraction which is transmitted towards theplane mirrored first surface comprised by the microelectromechanicalmirror which is attached to the third side of the storage container; andso to also produce a third reflected laser beam fraction which isreflected towards the laser output apparatus.

Wherein, the second reflected laser beam fraction and the thirdtransmitted laser beam fraction combine at the inner mirrored surface ofthe beam splitter, such that waves comprised by the combined laser beamfractions superimpose totally out of phase so to produce totaldestructive interference, and such that associated time-varying electricand magnetic fields comprised in the combined laser beam fractionstotally cancel respectively. Thus, the second reflected laser beamfraction and the third transmitted laser beam fraction combine toproduce a beam of totally electromagnetically neutralizedelectromagnetic field quanta (e.g., a beam of totallyelectromagnetically neutralized electromagnetic field quanta as the beamof totally electromagnetically neutralized wave-particle behavingentities shown in FIG. (3)). (Also, similarly, the second transmittedlaser beam fraction and the third reflected laser beam fraction combineat the beam splitter to produce an extraneous beam of totallyelectromagnetically neutralized electromagnetic field quanta.) Then, thebeam of totally electromagnetically neutralized electromagnetic fieldquanta, is coherently transmitted by the vacuum to the totallyreflecting microelectromechanical mirror which is attached to the thirdside so to impinge along a normal upon, and then totally reflect from,the totally reflecting plane mirrored first surface comprised by themicroelectromechanical mirror in a coherent manner. (Also, theextraneous beam of totally electromagnetically neutralizedelectromagnetic field quanta is effectively eliminated from the storagecontainer.)

Subsequently, the beam of totally electromagnetically neutralizedelectromagnetic field quanta is coherently transmitted by the vacuumback to the beam splitter which then reflects the beam of totallyelectromagnetically neutralized electromagnetic field quanta in acoherent manner along an angle such that the beam of totallyelectromagnetically neutralized electromagnetic field quanta iscoherently transmitted by the vacuum to the mirror which is comprised bythe second side of the storage container. (Here, the beam splitter iseffectively totally reflecting from inside the storage container, i.e.,is a significant potential energy barrier to the beam of totallyelectromagnetically neutralized electromagnetic field quanta.)

Then, the beam of totally electromagnetically neutralizedelectromagnetic field quanta impinges along a normal upon, and thentotally reflects coherently from, the totally reflecting plane mirroredfirst surface of the mirror which is attached to the second side of thestorage container. Subsequently, the beam of totally electromagneticallyneutralized electromagnetic field quanta is coherently transmitted bythe vacuum back to beam splitter where the coherent transmissionsequence began. Then, a repetition of the coherent transmission sequenceof the beam of totally electromagnetically neutralized electromagneticfield quanta occurs to repeatedly store energy.

Nevertheless, during coherent transmission, adverse electromagneticinteraction of the beam of electromagnetically neutralized wave-particlebehaving entities with electrically charged particles comprised in thecoherently transmitting storage container is eliminated to an extent.Hence, adverse electromagnetic effects of storing energy are eliminatedto an extent (e.g., the inefficiency of storing energy is eliminated toan extent).

Then, when the mirror (e.g., microelectromechanical mirror) is tilted(dashed line), the beam of electromagnetically neutralized wave-particlebehaving entities is coherently transmitted by the vacuum to an exitport which is incorporated in the beam splitter. Wherein, the beam ofelectromagnetically neutralized wave-particle behaving entities thenexits the storage container for utilization. (Note, the storage of abeam of totally electromagnetically neutralized wave-particle behavingatomic nuclei is not recommended as relates to the preferred embodimentdescribed herein because of the use of a beam of totallyelectromagnetically neutralized wave-particle behaving atomic nuclei,e.g., a beam of totally electromagnetically neutralized wave-particlebehaving protons, for cold nuclear fusion in the preferred embodiment inFIG. (30)).

FIG. (56A) shows a perspective view of the basic shape of the energystorage container which is applied in the preferred embodiment of thepresent invention in FIG. (56).

FIG. (57) shows a plan top view of a preferred embodiment of the presentinvention which is applied for efficient momentum-based voltagegeneration. FIG. (57) basically applies the steps applied in thepreferred embodiment in FIG. (56) with some modifications.

In the preferred embodiment in FIG. (57), apparatus, which comprisesMichelson interferometric apparatus, comprises a miniature laser (52)which produces a pulse laser beam (54). The pulsed laser beam (54) isdivided (i.e., partly transmitted and partly reflected) by the partiallymirrored second surface of the plane beam splitter (56) (i.e., a partlytransmitting and partly reflecting mirror) so to produce a firsttransmitted pulsed laser beam fraction, and so also to produce a firstreflected pulsed laser beam fraction. Here, the beam splitter (56) iscomprised by one side of an enclosed, sealed, storage container (58),which is a triangularly shaped pentahedron (five sided polyhedron) whichalso comprises the second side (60), the third side (62), the top andbottom sides (64) and (66), respectively, and contains the vacuum(evacuated space) (68).

Then, the first transmitted pulsed laser beam fraction is coherentlytransmitted by the vacuum (68) to the totally reflecting plane mirroredfirst surface comprised by the pressure transducer (70) (e.g., apiezoelectric based transducer), which is comprised by, for example, themicroelectromechanical device (MEMS device) (72) which is attached tothe inner side of the second side (60) of the storage container (58);and the first reflected pulsed laser beam fraction is transmitted by theair (or vacuum) (42T) to a totally reflecting plane mirrored firstsurface comprised by a mirror (74) which is separate from the storagecontainer (58). Then, the totally reflecting pressure transducer (70),which is attached to the second side (60), totally reflects the firsttransmitted pulsed laser beam fraction so that the first transmittedpulsed laser beam fraction is then coherently transmitted by the vacuum(68) back to the beam splitter (56), which then divides the firsttransmitted pulsed laser beam fraction so to produce a secondtransmitted pulsed laser beam fraction which is transmitted back towardsthe laser output apparatus; and so to produce a second reflected pulsedlaser beam fraction which is reflected towards the plane mirrored firstsurface of the third side (62) of the storage container (58). Also, thetotally reflecting mirror (74) totally reflects the first reflectedpulsed laser beam fraction so that the first reflected pulsed laser beamfraction is then coherently transmitted by the air (or vacuum) (42T)back to the beam splitter (56) which then divides the first reflectedpulsed laser beam fraction so to produce a third transmitted pulsedlaser beam fraction which is transmitted towards the plane mirroredfirst surface of the third side (62); and so to also produce a thirdreflected pulsed laser beam fraction which is reflected towards thelaser output apparatus.

Wherein, the second reflected pulsed laser beam fraction and the thirdtransmitted pulsed laser beam fraction combine at the inner mirroredsurface of beam splitter (56), such that waves comprised by the combinedpulsed laser beam fractions superimpose totally out of phase so toproduce total destructive interference, and such that associatedtime-varying electric and magnetic fields comprised in the combinedpulsed laser beam fractions totally cancel respectively. Thus, thesecond reflected pulsed laser beam fraction and the third transmittedpulsed laser beam fraction combine to produce the pulsed beam of totallyelectromagnetically neutralized electromagnetic field quanta (4T) (e.g.,a pulsed beam of totally electromagnetically neutralized electromagneticfield quanta as the beam of totally electromagnetically neutralizedwave-particle behaving entities shown in FIG. (4)). (Also, similarly,the second transmitted pulsed laser beam fraction and the thirdreflected pulsed laser beam fraction combine at the beam splitter toproduce an extraneous pulsed beam of totally electromagneticallyneutralized electromagnetic field quanta.) Then, the pulsed beam oftotally electromagnetically neutralized electromagnetic field quanta(4T), is coherently transmitted by the vacuum (68) to the totallyreflecting third side (62) so to impinge along a normal upon, and thentotally reflect from, the totally reflecting plane mirrored firstsurface of the third side (62). (Also, the extraneous pulsed beam oftotally electromagnetically neutralized electromagnetic field quanta iseffectively eliminated from the storage container (58).)

Subsequently, the pulse modulated beam of totally electromagneticallyneutralized electromagnetic field quanta (4T) is coherently transmittedby the vacuum (68) back to the beam splitter (56) which then reflectsthe pulsed beam of totally electromagnetically neutralizedelectromagnetic field quanta (4T) along an angle such that the pulsedbeam of totally electromagnetically neutralized electromagnetic fieldquanta (4T) is coherently transmitted by the vacuum (68) to the pressuretransducer (70). (Here, the beam splitter is effectively totallyreflecting from inside the storage container, i.e., is a significantpotential energy barrier to the pulsed beam of totallyelectromagnetically neutralized electromagnetic field quanta (4T).)

Then, the beam of totally electromagnetically neutralizedelectromagnetic field quanta (4T) impinges along a normal upon, and thentotally reflects coherently from, the totally reflecting plane mirroredfirst surface of the pressure transducer (70) (a momentum-type utilizingapparatus) so to impart momentum upon the pressure transducer and, ineffect, apply pressure upon the pressure transducer (for every pulse).Wherein, the pressure transducer transforms the applied pressure intovoltage (for every pulse) for utilization. (Note, the coherentlytransmitted beam of totally electromagnetically neutralizedelectromagnetic field quanta (4T) imparts momentum, i.e., appliespressure, upon the pressure transducer by a process in which thepressure transducer would utilize momentum by way of Newton's second lawof physics in which momentum would be applied to the pressure transducerby a momentum vector which is equal in magnitude and opposite indirection to the change of the momentum vector of the respectivelyreflected beam of totally electromagnetically neutralized wave-particlebehaving entities).

Subsequently, the pulse modulated beam of totally electromagneticallyneutralized electromagnetic field quanta (4T) is coherently transmittedby the vacuum (68) back to beam splitter (56) where the coherenttransmission sequence began. Then, a repetition of the coherenttransmission sequence of the beam of totally electromagneticallyneutralized electromagnetic field quanta (4T) occurs to repeatedlygenerate voltage. (Note, the pulse modulated beam of totallyelectromagnetically neutralized electromagnetic field quanta (4T) has alength which is equal to or less than the path length the beampropagates in one cycle of voltage generation (which includes asufficient gap in the stream of pulses, if a plurality of pulses isapplied, for the tilting of the microelectromechanical mirror in anenergy elimination process as described later), and a constantmodulation frequency; and the pressure transducer resonates at themodulation frequency of beam (4T).)

Nevertheless, during coherent transmission, adverse electromagneticinteraction of the beam of totally electromagnetically neutralizedelectromagnetic field quanta (4T) with electrically charged particlescomprised in the coherently transmitting container is totallyeliminated. Hence, certain adverse electromagnetic effects oftransmitting energy for voltage generation are totally eliminated (e.g.,the inefficiency of voltage generation due to adverse electromagneticeffects is totally eliminated).

Then, if the pressure transducer (70) comprised by themicroelectromechanical device (72) is tilted (dashed line), the beam oftotally electromagnetically neutralized electromagnetic field quanta(4U) is coherently transmitted by the vacuum (68) to the exit port (76),which is incorporated in the beam splitter (56), where the beam oftotally electromagnetically neutralized electromagnetic field quanta(4U) exits the storage container. Then, the beam of totallyelectromagnetically neutralized electromagnetic field quanta (4U) istransmitted by the exit port (76) to the eliminating apparatus (78).Wherein, eliminating apparatus (78) can comprise incoherently scatteringmedia which merely incoherently scatter the beam of totallyelectromagnetically neutralized electromagnetic field quanta (4U) inorder to eliminate the beam of totally electromagnetically neutralizedelectromagnetic field quanta (4U) for all practical purposes from thevoltage generation process; or, in addition, eliminating media cancomprise transmission media and electromagnetically absorptive media,such that electromagnetically functional electromagnetic field quanta(comprising a non-zero time-average electric flux density) which areproduced by incoherent scattering, can be transmitted by transmittingmedia to, and then absorbed by, electromagnetically absorptive media,comprising electrically charged particles, by way of electromagneticinteraction in the eliminating apparatus in order to eliminate theenergy from the voltage generating process. (Here, the eliminatingapparatus (78) can comprises potential-energy-type andelectromagnetic-type incoherently scattering and transmitting media, andelectromagnetically absorptive apparatus.)

FIG. (58) shows another preferred embodiment of the present inventionwhich is applied for efficient voltage generation. The steps applied inthe preferred embodiment in FIG. (57) are applied in the preferredembodiment in FIG. (58) except that apparatus, as described in thepreferred embodiment in FIG. (57), in addition, comprises additionalMichelson interferometric apparatus which produces a second pulsed beamof totally electromagnetically neutralized wave-particle behavingentities; a second microelectromechanical device comprising a respectivepressure transducer; and a second exit port with a respectiveeliminating apparatus. Wherein, the preferred embodiment in FIG. (58)shows how a plurality of voltage generating sources can be constructedwith one storage container by applying an equivalent method ofgenerating voltage for each pulsed beam of totally electromagneticallyneutralized wave-particle behaving entities applied (as described forthe pulse modulated beam of totally electromagnetically neutralizedwave-particle behaving entities in the preferred embodiment in FIG. 57).

FIG. (59) shows a preferred embodiment of the present invention which isapplied for efficient power generation. The steps applied in theembodiment in FIG. (58) are applied in the preferred embodiment in FIG.(59) except that apparatus, as described in the preferred embodiment inFIG. (57), in addition, comprises a load connected to the pressuretransducer, such that the voltage generator in FIG. (59) is now a powergenerator which provides power for the load.

FIG. (60) shows a preferred embodiment of the present invention which isapplied for data storage and retrieval in an efficient manner. In thiscase, the embodiment in FIG. (60) totally eliminates the adverseelectromagnetic interaction of electromagnetic field quanta with datastorage and retrieval media, hence totally eliminating the adverseelectromagnetic effects of data storage and retrieval due to adverseelectromagnetic interaction (e.g., totally eliminating the volatility ofdata storage and retrieval due to adverse electromagnetic interaction),and further provides for a dense and fast form of data storage andretrieval.

The steps applied in the embodiment in FIG. (57) are basically appliedin the preferred embodiment herein except that the method in thepreferred embodiment in FIG. (60) is a data storage and retrieval methodin which apparatus comprising Michelson interferometric apparatus, and apulse modulator, produces a pulse modulated beam of totallyelectromagnetically neutralized electromagnetic field quanta which ispulse modulated so as to encode data (e.g., pulse modulated so as toencode data as the beam in FIG. (5)). Wherein, the pulse modulated beamof totally electromagnetically neutralized electromagnetic field quantaapplied is coherently transmitted by the storage container and impartsmomentum, i.e., applies pressure, upon a momentum-type utilizingapparatus comprising a pressure transducer, and in effect appliespressure (for every pulse) upon the pressure transducer which iscomprised by a receiving apparatus. Wherein, the receiving apparatustransforms the applied pressure into voltages which encode data forquick retrieval. (Note, the coherently transmitted beam of totallyelectromagnetically neutralized electromagnetic field quanta impartsmomentum, i.e., applies pressure, upon the pressure transducer by aprocess in which the pressure transducer would utilize momentum by wayof Newton's second law of physics as mentioned in the preferredembodiment in FIG. 57). Furthermore, the modulated beam of totallyelectromagnetically neutralized electromagnetic field quanta can beeliminated from the data storage and retrieval apparatus by tilting therespectively applied pressure transducer (which is attached to amicroelectromechanical device) so that when the respectively reflectedmodulated beam of totally electromagnetically neutralizedelectromagnetic field quanta is eliminated from the data storage andretrieval apparatus (as the modulated beam of totallyelectromagnetically neutralized electromagnetic field quanta iseliminated from the data storage and retrieval apparatus in FIG. 57)data can be erased from data storage and retrieval apparatus (i.e., datacan be erased from memory).

Other preferred embodiments of the present invention for data storageand retrieval can provide for increased data storage capacity (andrespective data retrieval capacity) by providing certain aspectsincluding: a) increasing the size of the storage container so that thelength of the beam of totally electromagnetically neutralizedelectromagnetic field quanta can be longer, and thus the amount of datathat the applied beam of totally electromagnetically neutralizedelectromagnetic field quanta can encode can be greater; b) increasingthe frequency of the beam (or beams) which impinge upon the respectivelyapplied pressure transducer (or transducers); c) aligning therespectively applied reflecting surfaces, which are comprised byrespectively applied Michelson interferometric apparatus andrespectively applied pressure transducers, along angles so that the beamof totally electromagnetically neutralized electromagnetic field quantaapplied propagates in a zigzag manner such that the length of the beamof totally electromagnetically neutralized electromagnetic field quantaapplied can be longer, and thus the amount of data that the applied beamof totally electromagnetically neutralized electromagnetic field quantaencodes can be greater; d) applying a method in which a multiplicity ofbeams of totally electromagnetically neutralized electromagnetic fieldquanta are applied, and thus an embodiment can store (and respectivelyretrieve) a greater amount of data; e) aligning the respectively appliedreflecting surfaces, which are comprised by respectively appliedMichelson interferometric apparatus and respectively applied pressuretransducers, along different angles so that the beams of totallyelectromagnetically neutralized electromagnetic field quanta appliedeach propagate in a zigzag manner along a respective beam axis along adifferent angle from a respective beam vertical axis which increases inmagnitude for microelectromechanical devices which are positionedfurther from the center of the storage container, so that a given beamof totally electromagnetically neutralized electromagnetic field quantaapplied only impinges upon a respective pressure transducer andcorresponding Michelson interferometric apparatus (and misses impingingupon any other pressure transducer and Michelson interferometricapparatus), and so that the smaller the angle from the respectivevertical axis of a given pulse modulated beam of totallyelectromagnetically neutralized electromagnetic field quanta, thegreater the number of reflections and the longer the path length, andrespective length itself, of the given pulse modulated beam of totallyelectromagnetically neutralized electromagnetic field quanta, and thusthe greater the amount of data the given pulse modulated beam of totallyelectromagnetically neutralized electromagnetic field quanta can encode;and/or f) adding apparatus and respectively applied beams of totallyelectromagnetically neutralized electromagnetic field quanta which areapplied along other geometric planes. (Note, the preferred embodimentdescribed in FIGS. (61), (61A), and (62) are involved in the applicationof some of such methods of increasing data storage and retrievalcapacity comprised herein.)

FIG. (61) is a sectional view of another preferred embodiment of thepresent invention which is applied for data storage and retrieval in anefficient manner. The preferred embodiment in FIG. (61) is a modifiedversion of the preferred embodiment shown in FIG. (60) in that thepreferred embodiment in FIG. (61) has an increased data storage (andretrieval) capacity. The steps applied in the preferred embodiment inFIG. (61) are basically applied in the preferred embodiment shown inFIG. (57) except for the number and configuration of certain apparatuswhich are applied. FIG. (61) shows more detail of only a certain limitedamount of apparatus which is actually present in the cubic shaped datastorage and retrieval apparatus shown in FIG. (61).

In the preferred embodiment in FIG. (61), first and second transmitterapparatus (which are comprised in the top of the storage container) andthird and fourth transmitter apparatus (which are comprised in thebottom of the storage container), each comprise respective Michelsonapparatus, and produce a first, second, third, and fourth pulsemodulated beam of totally electromagnetically neutralizedelectromagnetic field quanta, respectively. Wherein, each pulsemodulated beam of totally electromagnetically neutralizedelectromagnetic field quanta encodes data (e.g., as the pulse modulatedbeam of totally electromagnetically neutralized wave-particle behavingentities shown in FIG. (5)).

Then, the first and second pulse modulated beams of totallyelectromagnetically neutralized electromagnetic field quanta are eachcoherently transmitted by the vacuum and the totally reflecting firstsurface plane mirrors, which are positioned between the transmitter andreceiver apparatus on respective top and bottom sides of the storagecontainer, to a respective totally reflecting pressure transducer (e.g.,a totally reflecting piezoelectric-based transducer), which are eachtotally reflecting at the first surface and are incorporated in fifthand sixth receiver apparatus (which are incorporated into the top sideof the storage container), respectively; and the third and fourth pulsemodulated beams of totally electromagnetically neutralizedelectromagnetic field quanta are each coherently transmitted by thevacuum and the totally reflecting first surface plane mirrors, which arepositioned between the transmitter and receiver apparatus on respectivetop and bottom sides of the storage container, to a respective totallyreflecting pressure transducer (e.g., a totally reflectingpiezoelectric-based transducer), which are each totally reflecting atthe first surface and are incorporated in seventh and eighth receiverapparatus (which are incorporated into the bottom side of the storagecontainer), respectively.

Wherein, the first, second, third, and fourth pulse modulated beams oftotally electromagnetically neutralized electromagnetic field quantaeach impinge upon, and then totally reflect coherently from, the totallyreflecting first surface of a respective pressure transducer comprisedby a respective microelectromechanical device comprised by a respectivereceiver so to impart momentum upon a respective momentum-type utilizingapparatus comprising a respective pressure transducer and, in effect,apply pressure upon the respective pressure transducer (for every pulse)which transforms the applied pressure into voltage for data retrieval.(Note, the coherently transmitted beam of totally electromagneticallyneutralized electromagnetic field quanta imparts momentum, i.e., appliespressure, upon the pressure transducer by a process in which a pressuretransducer would utilize momentum by way of Newton's second law ofphysics as mentioned in the preferred embodiment in FIG. 57).

Subsequently, the first, second, third, and fourth pulse modulated beamsof totally electromagnetically neutralized electromagnetic field quantaare coherently transmitted by the vacuum (evacuated space) and thetotally reflecting mirrors (positioned between the transmitter andreceiver apparatus respectively incorporated in the top and bottom sidesof the storage container), back to and then reflected from, a respectiveMichelson interferometric apparatus (i.e., totally reflected by arespective plane beam splitter and effective totally reflecting secondside (as relates to the preferred embodiment in FIG. 57). (Note, thebeam splitter is totally reflecting from inside the storage container,i.e., is a significant potential energy barrier to the respectivelyimpinging beam of totally electromagnetically neutralizedelectromagnetic field quanta, and effective totally reflecting secondside as relates to the preferred embodiments in FIGS. (56) and (57).Also, note that here transmitter and receiver apparatus comprising aMichelson interferometric apparatus and a corresponding pressuretransducer, respectively, are each aligned along an angle from arespective vertical axis which increases in magnitude for transmitterand receiver apparatus which are positioned further from the center ofthe storage container. Wherein, each pulse modulated beam of totallyelectromagnetically neutralized electromagnetic field quanta propagatesalong a respective beam axis along an angle from a respective verticalaxis which increases in magnitude for transmitter and receiver apparatuswhich are positioned further from the center of the storage container,so that a given beam of totally electromagnetically neutralizedelectromagnetic field quanta applied only impinges upon a respectivepressure transducer and corresponding Michelson interferometricapparatus, and so that the smaller the angle from the respectivevertical axis of a given pulse modulated beam of totallyelectromagnetically neutralized electromagnetic field quanta, thegreater the number of reflections and the longer the path length, andrespective length itself, of a given pulse modulated beam of totallyelectromagnetically neutralized electromagnetic field quanta, and thusthe greater the amount of data the given pulse modulated beam of totallyelectromagnetically neutralized electromagnetic field quanta can encode.Furthermore, note that the pulse modulated beams of totallyelectromagnetically neutralized electromagnetic field quanta each have alength which is equal to or less than the path length the beampropagates in one cycle of data storage so that the data does notoverlap and is distinguishable by a respective receiving apparatus, andalso each comprise a sufficient gap in the data stream if the tilting ofa comprised in respective receiver apparatus is applied for the erasureof data from the data storage and retrieval apparatus as describedlater.) Then, a repetition of the coherent transmission sequence of thefirst, second, third, and fourth pulse modulated beams of totallyelectromagnetically neutralized electromagnetic field quanta occurs torepeatedly generate a voltage, which encodes data, and which isavailable for quick retrieval.

Nevertheless, during coherent transmission, adverse electromagneticinteraction of the pulse modulated beams of totally electromagneticallyneutralized electromagnetic field quanta with electrically chargedparticles comprised in the coherently transmitting storage container istotally eliminated. Hence, certain adverse electromagnetic effects oftransmitting energy for data storage and retrieval are totallyeliminated (e.g., the electromagnetic volatility of data storage andretrieval is totally eliminated).

Then, if the microelectromechanical device comprised in the fifth,sixth, seventh, and/or eighth receiver apparatus are tilted, then thefirst, second, third, and/or fourth pulse modulated beams of totallyelectromagnetically neutralized electromagnetic field quanta,respectively, are coherently transmitted by the vacuum to a respectiveexit port comprising a first, second, third, and fourth exit port,respectively, where the first, second, third, and/or fourth pulsemodulated beams of totally electromagnetically neutralizedelectromagnetic field quanta would exit the storage container. Then, thefirst, second, third, and/or fourth pulse modulated beams of totallyelectromagnetically neutralized electromagnetic field quanta would betransmitted by a respective exit port to a first, second, third, andfourth eliminating apparatus, respectively. Wherein, eliminatingapparatus can comprise incoherently scattering media which can merelyincoherently scatter the respectively applied pulse modulated beam oftotally electromagnetically neutralized electromagnetic field quanta inorder to eliminate the respective pulse modulated beam of totallyelectromagnetically neutralized electromagnetic field quanta for allpractical purposes in order to erase data from the data storage andretrieval apparatus (i.e., erase data from memory); or, in addition,eliminating apparatus can comprise transmission media andelectromagnetically absorptive apparatus, such that electromagneticallyfunctional electromagnetic field quanta (comprising a non-zerotime-average electric flux density), which are produced by incoherentscattering, can be transmitted by transmitting media to, and thenabsorbed by, electromagnetically absorptive media, comprisingelectrically charged particles, by way of electromagnetic interaction ineliminating apparatus in order to erase data from the data storage andretrieval apparatus (i.e., erase data from memory). (Here, theeliminating apparatus comprises potential-energy-type incoherentlyscattering media and electromagnetic-type incoherently scattering media,and electromagnetically absorptive media.)

Herein, FIG. (61) only selectively shows a certain limited amount of theapparatus which is actually present in the data storage and retrievalapparatus shown in FIG. (61) including only the pulse modulated beams oftotally electromagnetically neutralized electromagnetic field quantawhich propagate within one of a multiplicity of planes which areparallel to the side of the apparatus shown in FIG. (61). However, otherequivalent apparatus in the preferred embodiment in FIG. (61) produceother equivalent pulse modulated beams of totally electromagneticallyneutralized electromagnetic field quanta which propagate in the sameplane, other planes which are parallel to the same side, and otherplanes which are parallel to other sides of the cubic shaped datastorage and retrieval apparatus (shown in FIG. (61) which provides forgreater data (and respective retrieval) capacity.

FIG. (61A) shows more detail of an enlarged view of a section of thepreferred embodiment for data storage and retrieval shown in FIG. (61)which exclusively shows one Michelson interferometric apparatuscomprising a plane beam splitter and effective second side applied inthe preferred embodiment in FIG. (61) (as described in the preferredembodiment in FIG. 57 in more detail). Wherein, the given beam oftotally electromagnetically neutralized electromagnetic field quantashown is reflected from a respective Michelson interferometric apparatusat a respective beam splitter and effective second side.

FIG. (62) shows another preferred embodiment of the present inventionwhich is applied for data storage and retrieval in an efficient manner.The steps applied in the embodiment in FIG. (61) are basically appliedin the preferred embodiment in FIG. (62) except with some modifications.

In the preferred embodiment in FIG. (62), each transmitter apparatus,which comprises Michelson interferometric apparatus and a laser, isamplitude modulated at different modulating frequencies so that eachrespective transmitter apparatus can produce amplitude modulated laserbeams of different frequencies. Wherein, in effect, each transmitterapparatus can produce a multiplexed beam of totally electromagneticallyneutralized electromagnetic field quanta comprising a plurality ofamplitude modulated beams of totally electromagnetically neutralizedelectromagnetic field quanta of different modulated frequencies (i.e., atype of frequency division multiplexed beam of totallyelectromagnetically neutralized electromagnetic field quanta). FIG. (5)shows one such amplitude modulated beam except that the beam applied inthe preferred embodiment herein more specifically applies a beam oftotally electromagnetically neutralized electromagnetic field quanta.

In this case, each multiplexed beam of totally electromagneticallyneutralized electromagnetic field quanta is coherently transmitted bycoherent transmission media in the storage container to a plurality ofseparate receiver apparatus which each comprise a microelectromechanicaldevice comprising a tunable pressure transducer which comprises arespective resonant frequency. Wherein, each tuned pressure transducer,which is comprised by a receiving apparatus, isolates a certainfrequency corresponding to a certain beam of totally electromagneticallyneutralized electromagnetic field quanta in the multiplexed beam oftotally electromagnetically neutralized electromagnetic field quantawhich impinges upon the respective pressure transducer comprised in arespective receiving apparatus. Hence, a respective pressure transducerproduces voltages (which encode data) from the effectively isolatedpressure pulses of a certain frequency which are applied by a respectivebeam of totally electromagnetically neutralized electromagnetic fieldquanta to the respective pressure transducer.

Here, the tuned pressure transducers which receive one commonmultiplexed beam of totally electromagnetically neutralizedelectromagnetic field quanta collective act as a type of demultiplexer.In effect, the preferred embodiment in FIG. (62) is electromagneticallynon-volatile and has a high density of data stored which is availablefor quick retrieval.

(Notes: Reference numbers are even numbers starting with (2); if a givenreference number includes a letter (or letters) following a number, thenthe number represents the group of closely related parts to which theparticular part belongs, and the letter following the number representsa particular version of the part within the respective group; if a givenfigure includes a letter then the number represents the group of closelyrelated figures to which the given figure belongs, and the letterfollowing the number represents the particular version of the figurewithin the respective group; the capital letters (D), (I), (O), and (Q)are neither used as letters following a reference number nor as aletters following a number in a figure number so as not to be confusedwith the numbers zero and one as respectively applicable; if a referencenumber includes a letter, in some cases, the respective letter may nothave, in sequential order, a preceding letter and/or may not have, insequential order, a succeeding letter because each such letter which isassociated with reference numbers is associated with a particularembodiment of the present invention in attempt to minimize confusion; abeam of electromagnetically neutralized wave-particle behaving entitiesis not considered to be hidden in a drawing where it is shown, and thusa beam of electromagnetically neutralized wave-particle behavingentities is not represented by a dashed line in such cases; referencesto a position located anterior to a given object pertains to a locationwhich is positioned proximal to the source of the given beam appliedrelative to the given object in a respective embodiment; references to aposition located posterior to a given object pertains to a locationwhich is positioned distal to the source of the given beam appliedrelative to the given object in a respective embodiment; anelectromagnetically neutralized beam means a beam which iselectromagnetically neutralized to an extent, i.e., electromagneticallyneutralized to a full extent or electromagnetically neutralized to apartial extent; the total destructive interference of waves and therespective total cancellation of electric and magnetic fields areabsolute terms and may not be actually producible under certainconditions; herein, various forms of the term transmit (e.g., transmits,transmitted, transmission, transmitting, etc.) refer respectively tovarious corresponding forms of the term convey, such that, for example,the term transmission refers to the process of transmission which caninclude scattering, backscattering, deflection, reflection, andrefraction in order to convey energy in a targeted direction; certainbeams of wave-particle behaving entities (e.g., one or more beams of oneor more wave-particle behaving entities, which may be created by, e.g.,backreflections; multiple, e.g., secondary, reflections; or extraneousbeams, in any given embodiment in the specification herein may neitherbe shown nor referred to in some way or ways so that any such embodimentof the present invention is not too confusing; one should be aware ofthe use of a beam of totally electromagnetically neutralizedwave-particle behaving atomic nuclei, e.g., a beam of totallyelectromagnetically neutralized wave-particle behaving protons, for coldnuclear fusion as described in the preferred embodiment in FIG. (30),before choosing a beam of electromagnetically neutralized wave-particlebehaving entities to be applied for any given application of the presentinvention; and the present invention is intended to be used according tothe laws which govern the use of such inventions.)

The detailed description of the present invention herein describes alimited number of the embodiments of the present invention. Yet, variousother embodiments of the present invention can be included in the scopeof the present invention. Thus, the present invention should beinterpreted in as broad a scope as possible so as to include all theequivalent embodiments of the present invention.

1. Method of transmitting energy, wherein the new use comprises: Step 1)providing apparatus for producing a beam of neutralized wave-particlebehaving means which comprise energy and oscillating means ofinteracting which are neutralized to an extent; and, Step 2) coherenttransmission of said beam of neutralized wave-particle behaving means toa target providing means by coherently transmitting means whichcomprises means of interacting with oscillating means of interactingwhich is functional to an extent; thereby, adverse interaction of saidoscillating means of interacting which are neutralized to an extent withsaid means of interacting with oscillating means of interacting which isfunctional to an extent is thus eliminated to an extent, and thereby theadverse effect of transmitting energy is eliminated to an extent,whereby energy is transmitted to said target providing means in aneffective manner to accomplish the objective of the method oftransmitting energy.